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Physics Midterm Review 2012. Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance.

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Presentation on theme: "Physics Midterm Review 2012. Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance."— Presentation transcript:

1 Physics Midterm Review 2012

2 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

3 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

4 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

5 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

6 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

7 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

8 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

9 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

10 Terms - Measurements time elapsed = duration of an event – there is a beginning, a middle, and an end to any event. distance = path length displacement = change in position mass = measure of inertia or resistance to change in state of motion

11 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

12 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

13 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

14 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

15 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

16 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

17 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

18 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

19 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

20 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

21 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

22 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

23 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

24 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

25 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

26 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

27 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

28 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

29 Calculated Values speed – distance as a function of time velocity – change in position as a function of time acceleration – change in velocity as a function of time centripetal acceleration – Quotient of the velocity squared and the distance from the center of rotation momentum – product of mass and velocity change in momentum = Impulse = change in the product of mass and velocity force = change in momentum per unit of time

30 Calculated Values Weight = Force due to Gravity = product of mass and acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

31 Calculated Values Weight = Force due to Gravity = product of mass and acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

32 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

33 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

34 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

35 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

36 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

37 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

38 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

39 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

40 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

41 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

42 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

43 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

44 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

45 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

46 Calculated Values Weight = Force due to Gravity = product of massand acceleration due to gravity Universal Gravitational Force is directly proportional to the universal gravitational constant, the mass of one object, the mass of another object and inversely proportional to the distance between the center of the objects squared work – product of parallel component of the force and distance the force is applied through Kinetic energy – product of ½ the mass and the velocity squared.

47 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

48 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

49 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

50 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

51 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

52 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

53 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

54 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

55 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

56 Calculated Values Power = work done per unit of time Power = energy transferred per unit of time Pressure= Force per unit area Torque = product of perpendicular component of force and distance the force is applied to the center of rotation moment of Inertia – sum of the product of the mass and the distance from the center of rotation squared

57 Mechanics Final velocity = initial velocity added to the product of the acceleration and time accelerating. Formula: v = v o + at Units: m = m + m (s) s s s 2 Relationships: Therefore the final velocity is directly related to the acceleration. It is also directly related to the time accelerating.

58 Mechanics Final velocity = initial velocity added to the product of the acceleration and time accelerating. Formula: v = v o + at Units: m = m + m (s) s s s 2 Relationships: Therefore the final velocity is directly related to the acceleration. It is also directly related to the time accelerating.

59 Mechanics Final velocity = initial velocity added to the product of the acceleration and time accelerating. Formula: v = v o + at Units: m = m + m (s) s s s 2 Relationships: Therefore the final velocity is directly related to the acceleration. It is also directly related to the time accelerating.

60 Mechanics Final velocity = initial velocity added to the product of the acceleration and time accelerating. Formula: v = v o + at Units: m = m + m (s) s s s 2 Relationships: Therefore the final velocity is directly related to the acceleration. It is also directly related to the time accelerating.

61 Mechanics Final velocity = initial velocity added to the product of the acceleration and time accelerating. Formula: v = v o + at Units: m = m + m (s) s s s 2 Relationships: Therefore the final velocity is directly related to the acceleration. It is also directly related to the time accelerating.

62 Mechanics Final position is equal to the initial position added to the product of the initial velocity and the time elapsed and the one half the product of the acceleration and time accelerating squared Formula x=x o + v o t + ½ at 2 Units m =m + m (s) m s 2 s s 2 The displacement is equal to the product of the initial velocity and the time elasped and the one half the product of the acceleration and time accelerating squared Formula  x = v o t + ½ at 2 Units m =m (s) m s 2 s s 2 If the initial velocity is zero the displacement is directly related to the square of the time accelerating

63 Mechanics Final position is equal to the initial position added to the product of the initial velocity and the time elapsed and the one half the product of the acceleration and time accelerating squared Formula x=x o + v o t + ½ at 2 Units m =m + m (s) + m s 2 s s 2 The displacement is equal to the product of the initial velocity and the time elasped and the one half the product of the acceleration and time accelerating squared Formula  x = v o t + ½ at 2 Units m =m (s) m s 2 s s 2 If the initial velocity is zero the displacement is directly related to the square of the time accelerating

64 Mechanics Final position is equal to the initial position added to the product of the initial velocity and the time elapsed and the one half the product of the acceleration and time accelerating squared Formula x=x o + v o t + ½ at 2 Units m =m + m (s) + m s 2 s s 2 The displacement is equal to the product of the initial velocity and the time elasped and the one half the product of the acceleration and time accelerating squared Formula  x = v o t + ½ at 2 Units m =m (s) m s 2 s s 2 If the initial velocity is zero the displacement is directly related to the square of the time accelerating

65 Mechanics Final position is equal to the initial position added to the product of the initial velocity and the time elapsed and the one half the product of the acceleration and time accelerating squared Formula x=x o + v o t + ½ at 2 Units m =m + m (s) + m s 2 s s 2 The displacement is equal to the product of the initial velocity and the time elapsed and the one half the product of the acceleration and time accelerating squared Formula  x = v o t + ½ at 2 Units m =m (s) m s 2 s s 2 If the initial velocity is zero the displacement is directly related to the square of the time accelerating

66 Mechanics Final position is equal to the initial position added to the product of the initial velocity and the time elapsed and the one half the product of the acceleration and time accelerating squared Formula x=x o + v o t + ½ at 2 Units m =m + m (s) + m s 2 s s 2 The displacement is equal to the product of the initial velocity and the time elapsed and one half the product of the acceleration and time accelerating squared Formula  x = v o t + ½ at 2 Units m =m (s) m s 2 s s 2 If the initial velocity is zero the displacement is directly related to the square of the time accelerating

67 Mechanics Final Velocity Squared equals the Initial velocity squared added to the product of the acceleration and the displacement. Formula: v 2 = v o 2 + 2 a  x m 2 m 2 m m s 2 s 2 s 2 Very Useful because the relationships between final velocity, initial velocity, acceleration and displacement can be determined without knowing the time elasped

68 Mechanics Final Velocity Squared equals the Initial velocity squared added to the product of the acceleration and the displacement. Formula: v 2 = v o 2 + 2 a  x m 2 m 2 m m s 2 s 2 s 2 Very Useful because the relationships between final velocity, initial velocity, acceleration and displacement can be determined without knowing the time elasped

69 Mechanics Final Velocity Squared equals the Initial velocity squared added to the product of the acceleration and the displacement. Formula: v 2 = v o 2 + 2 a  x m 2 m 2 m m s 2 s 2 s 2 Very Useful because the relationships between final velocity, initial velocity, acceleration and displacement can be determined without knowing the time elasped

70 Mechanics Final Velocity Squared equals the Initial velocity squared added to the product of the acceleration and the displacement. Formula: v 2 = v o 2 + 2 a  x m 2 m 2 m m s 2 s 2 s 2 Very Useful because the relationships between final velocity, initial velocity, acceleration and displacement can be determined without knowing the time elasped

71 Mechanics Vector sum of the forces is equal to the net force which is equal to the product of the mass of the object and its acceleration. Formula:  F = F net = m a Units: N = kg m s 2 Noncontact – Gravitational, Electromagnetism, Nuclear Contact – Normal, Friction, Tension

72 Mechanics Vector sum of the forces is equal to the net force which is equal to the product of the mass of the object and its acceleration. Formula:  F = F net = m a Units: N = kg m s 2 Noncontact – Gravitational, Electromagnetism, Nuclear Contact – Normal, Friction, Tension

73 Mechanics Vector sum of the forces is equal to the net force which is equal to the product of the mass of the object and its acceleration. Formula:  F = F net = m a Units: N = kg m s 2 Noncontact – Gravitational, Electromagnetism, Nuclear Contact – Normal, Friction, Tension

74 Mechanics Vector sum of the forces is equal to the net force which is equal to the product of the mass of the object and its acceleration. Formula:  F = F net = m a Units: N = kg m s 2 Noncontact – Gravitational, Electromagnetism, Nuclear Contact – Normal, Friction, Tension

75 Mechanics Vector sum of the forces is equal to the net force which is equal to the product of the mass of the object and its acceleration. Formula:  F = F net = m a Units: N = kg m s 2 Noncontact – Gravitational, Electromagnetism, Nuclear Contact – Normal, Friction, Tension

76 Mechanics Vector sum of the forces is equal to the net force which is equal to the product of the mass of the object and its acceleration. Formula:  F = F net = m a Units: N = kg m s 2 Noncontact – Gravitational, Electromagnetism, Nuclear Contact – Normal, Friction, Tension

77 Mechanics Force due to friction is less than or equal to the product of the coefficient of friction and the normal force Formula F fr <  F N Units N N Therefore – Coefficient of friction is equal to the ratio of the normal force to the frictional force Formula  = F fr F N Units  = None – it is a ratio of the frictional force to the normal force

78 Mechanics Force due to friction is less than or equal to the product of the coefficient of friction and the normal force Formula F fr <  F N Units N N Therefore – Coefficient of friction is equal to the ratio of the normal force to the frictional force Formula  = F fr F N Units  = None – it is a ratio of the frictional force to the normal force

79 Mechanics Force due to friction is less than or equal to the product of the coefficient of friction and the normal force Formula F fr <  F N Units N N Therefore – Coefficient of friction is equal to the ratio of the normal force to the frictional force Formula  = F fr F N Units  = None – it is a ratio of the frictional force to the normal force

80 Mechanics Force due to friction is less than or equal to the product of the coefficient of friction and the normal force Formula F fr <  F N Units N N Therefore – Coefficient of friction is equal to the ratio of the normal force to the frictional force Formula  = F fr F N Units  = None – it is a ratio of the frictional force to the normal force

81 Mechanics Force due to friction is less than or equal to the product of the coefficient of friction and the normal force Formula F fr <  F N Units N N Therefore – Coefficient of friction is equal to the ratio of the normal force to the frictional force Formula  = F fr F N Units  = None – it is a ratio of the frictional force to the normal force

82 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

83 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

84 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

85 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

86 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

87 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

88 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

89 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

90 Mechanics Centripetal Acceleration is quotient of the velocity squared and the radius of its path Formula: a c = v 2 r Units m = (m/s) 2 s 2 m The magnitude of the velocity does not change The direction of the object continually changes towards the center of rotation The velocity vector is directed tangent to its path The acceleration vector is directed to the center of rotation The force vector that causes this motion is perpendicular to the velocity vector. The force vector is also directed towards the center of rotation

91 Mechanics The Torque is equal to the product of the force, distance that force is applied to the center of rotation and the sin of the angle that force is applied Formula  = F r sin  Units N m = N m No work is done because the force is applied perpendicular to the displacement

92 Mechanics The Torque is equal to the product of the force, distance that force is applied to the center of rotation and the sin of the angle that force is applied Formula  = F r sin  Units N m = N m No work is done because the force is applied perpendicular to the displacement

93 Mechanics The Torque is equal to the product of the force, distance that force is applied to the center of rotation and the sin of the angle that force is applied Formula  = F r sin  Units N m = N m No work is done because the force is applied perpendicular to the displacement

94 Mechanics The Torque is equal to the product of the force, distance that force is applied to the center of rotation and the sin of the angle that force is applied Formula  = F r sin  Units N m = N m No work is done because the force is applied perpendicular to the displacement

95 Mechanics The Torque is equal to the product of the force, distance that force is applied to the center of rotation and the sin of the angle that force is applied Formula  = F r sin  Units N m = N m No work is done because the force is applied perpendicular to the displacement

96 Mechanics Momentum equals the product of the mass and the velocity of the object Formula p = m v Units kg m = kg m s s Momentum before equals momentum after p o =p Called the conservation of momentum

97 Mechanics Momentum equals the product of the mass and the velocity of the object Formula p = m v Units kg m = kg m s s Momentum before equals momentum after p o =p Called the conservation of momentum

98 Mechanics Momentum equals the product of the mass and the velocity of the object Formula p = m v Units kg m = kg m s s Momentum before equals momentum after p o =p Called the conservation of momentum

99 Mechanics Momentum equals the product of the mass and the velocity of the object Formula p = m v Units kg m = kg m s s Momentum before equals momentum after p o =p Called the conservation of momentum

100 Mechanics Momentum equals the product of the mass and the velocity of the object Formula p = m v Units kg m = kg m s s Momentum before equals momentum after p o =p Called the conservation of momentum

101 Mechanics Impulse equals the change in momentum equals the product of the Force and the time that force acts. Formula J = F  t =  p Units Ns = N s = kg m s Force equals the quotient of the change in momentum and the time the force acts on the object Formula F =  p t Units N = kg m = kg m s s s 2

102 Mechanics Impulse equals the change in momentum equals the product of the Force and the time that force acts. Formula J = F  t =  p Units N s = N s = kg m s Force equals the quotient of the change in momentum and the time the force acts on the object Formula F =  p t Units N = kg m = kg m s s s 2

103 Mechanics Impulse equals the change in momentum equals the product of the Force and the time that force acts. Formula J = F  t =  p Units N s = N s = kg m s Force equals the quotient of the change in momentum and the time the force acts on the object Formula F =  p t Units N = kg m = kg m s s s 2

104 Mechanics Impulse equals the change in momentum equals the product of the Force and the time that force acts. Formula J = F  t =  p Units N s = N s = kg m s Force equals the quotient of the change in momentum and the time the force acts on the object Formula F =  p t Units N = kg m = kg m s s s 2

105 Mechanics Kinetic energy equals one half the product of the mass and the velocity squared of the object Formula k = ½ mv 2 Units J = kg m 2 = N m s 2 Relationship The kinetic energy varies directly as the square of the velocity Kinetic Energy is a scalar quantity

106 Mechanics Kinetic energy equals one half the product of the mass and the velocity squared of the object Formula k = ½ mv 2 Units J = kg m 2 = N m s 2 Relationship The kinetic energy varies directly as the square of the velocity Kinetic Energy is a scalar quantity

107 Mechanics Kinetic energy equals one half the product of the mass and the velocity squared of the object Formula k = ½ mv 2 Units J = kg m 2 = N m s 2 Relationship The kinetic energy varies directly as the square of the velocity Kinetic Energy is a scalar quantity

108 Mechanics Kinetic energy equals one half the product of the mass and the velocity squared of the object Formula k = ½ mv 2 Units J = kg m 2 = N m s 2 Relationship The kinetic energy varies directly as the square of the velocity Kinetic Energy is a scalar quantity

109 Mechanics Kinetic energy equals one half the product of the mass and the velocity squared of the object Formula k = ½ mv 2 Units J = kg m 2 = N m s 2 Relationship The kinetic energy varies directly as the square of the velocity Kinetic Energy is a scalar quantity

110 Mechanics Change in gravitational potential energy is equal to the product of the objects mass, acceleration due to gravity, and the vertical displacement of the object. Formula  U g = m g  y Units J = kg m m s 2 The gravitation potential energy equals the product of the mass, acceleration due to gravity, and the vertical position of the object.

111 Mechanics Change in gravitational potential energy is equal to the product of the objects mass, acceleration due to gravity, and the vertical displacement of the object. Formula  U g = m g  y Units J = kg m m s 2 The gravitation potential energy equals the product of the mass, acceleration due to gravity, and the vertical position of the object.

112 Mechanics Change in gravitational potential energy is equal to the product of the objects mass, acceleration due to gravity, and the vertical displacement of the object. Formula  U g = m g  y Units J = kg m m s 2 The gravitation potential energy equals the product of the mass, acceleration due to gravity, and the vertical position of the object.

113 Mechanics Change in gravitational potential energy is equal to the product of the objects mass, acceleration due to gravity, and the vertical displacement of the object. Formula  U g = m g  y Units J = kg m m s 2 The gravitation potential energy equals the product of the mass, acceleration due to gravity, and the vertical position of the object.

114 Mechanics Work is equal the product of the force the distance the object moves and the cosine of the angle the force is applied. Formula: W = F d cos  Units: J = N m = kg m m s 2

115 Mechanics Work is equal the product of the force the distance the object moves and the cosine of the angle the force is applied. Formula: W = F d cos  Units: J = N m = kg m m s 2

116 Mechanics Work is equal the product of the force the distance the object moves and the cosine of the angle the force is applied. Formula: W = F d cos  Units: J = N m = kg m m s 2

117 Mechanics Work is equal the product of the force the distance the object moves and the cosine of the angle the force is applied. Formula: W = F d cos  Units: J = N m = kg m m s 2

118 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

119 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

120 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

121 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

122 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

123 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

124 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 s Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

125 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 s Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

126 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 s Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

127 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 s Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

128 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 s Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

129 Mechanics Power is equal to the quotient of the work and the time the work is done in. Formula P = W t Power is equal to the quotient of the energy transferred and the time the energy is transferred in. Formula P =  U or  k t t Units Watts = Joules = N m = kg m m sec s s 2 s Power is equal to the product of the average force multiplied, the velocity of the object, and the cos of the angle that the force is applied. Formula P = F v cos  Units Watts = N m = J = kg m m s s s 2 s Units Work done or Energy Transferred equals the product of the Power and time the work is done in or energy is transferred in Formula Work = Power x time or Energy = Power x time U = P t W=Pt  k=Pt Units J = = Watts sec

130 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

131 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

132 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

133 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

134 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

135 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

136 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

137 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

138 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

139 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

140 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

141 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

142 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

143 Mechanics Restorative Force of a Spring is equal to the negative product of the spring constant and the displacement Formula F s = - Kx Units N N m m Potential energy associated with a spring is equal to one half the product of the spring constant and the displacement squared. Formula U s = ½ k x 2 Units Joule(J) = N m 2 = N m m The Period of Oscillation of a spring is equal to the product of 2  and the quotient of the square root of the mass attached to the spring and the spring constant Formula T s = 2  m Units = sec = kg or kg m or kg m or s 2 k N N kg m m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

144 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

145 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

146 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

147 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

148 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

149 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

150 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

151 Mechanics The period of oscillation of a pendulum is equal to the product of 2 p and the square root of the quotient of the length of the pendulum and the acceleration due to gravity. Formula T p = 2  l Units = sec = m or s 2 g m s 2 The Period of Oscillation is inversely proportional to its frequency Formula T = 1 f Units sec = 1 or 1 hz (cycle) sec

152 Mechanics The force due to gravity is equal quotient of the the product of the universal gravitational constant the, mass of one object, mass of a second object and the distance between the objects squared Formula F g = G mm r 2 Units N = 6.67x10 -11 N m 2 kg kg kg 2 m 2 The Weight which equals the force due to gravity near the surface of a planet is equal to the product of the mass and the acceleration due to gravity Formula W = F g = mg Units N = N = kg m s 2

153 Mechanics The force due to gravity is equal quotient of the the product of the universal gravitational constant the, mass of one object, mass of a second object and the distance between the objects squared Formula F g = G mm r 2 Units N = 6.67x10 -11 N m 2 kg kg kg 2 m 2 The Weight which equals the force due to gravity near the surface of a planet is equal to the product of the mass and the acceleration due to gravity Formula W = F g = mg Units N = N = kg m s 2

154 Mechanics The force due to gravity is equal quotient of the the product of the universal gravitational constant the, mass of one object, mass of a second object and the distance between the objects squared Formula F g = G mm r 2 Units N = 6.67x10 -11 N m 2 kg kg kg 2 m 2 The Weight which equals the force due to gravity near the surface of a planet is equal to the product of the mass and the acceleration due to gravity Formula W = F g = mg Units N = N = kg m s 2

155 Mechanics The force due to gravity is equal quotient of the the product of the universal gravitational constant the, mass of one object, mass of a second object and the distance between the objects squared Formula F g = G mm r 2 Units N = 6.67x10 -11 N m 2 kg kg kg 2 m 2 The Weight which equals the force due to gravity near the surface of a planet is equal to the product of the mass and the acceleration due to gravity Formula W = F g = mg Units N = N = kg m s 2

156 Mechanics The gravitational potential energy is equal quotient of the product of the universal gravitational constant the, mass of one object, mass of a secondobject and the distance between the objects Formula U g = G mm r Units Joules= 6.67x10 -11 N m 2 kg kg = N m kg 2 m The gravitational potential energy near the surface of a planet is equal to the product of the mass and the acceleration due to gravity and the vertical position of the object. Formula U g = m g y Units:Joules = kg m m= N m s 2

157 Mechanics The gravitational potential energy is equal quotient of the product of the universal gravitational constant the, mass of one object, mass of a secondobject and the distance between the objects Formula U g = G mm r Units Joules= 6.67x10 -11 N m 2 kg kg = N m kg 2 m The gravitational potential energy near the surface of a planet is equal to the product of the mass and the acceleration due to gravity and the vertical position of the object. Formula U g = m g y Units:Joules = kg m m= N m s 2

158 Mechanics The gravitational potential energy is equal quotient of the product of the universal gravitational constant the, mass of one object, mass of a secondobject and the distance between the objects Formula U g = G mm r Units Joules= 6.67x10 -11 N m 2 kg kg = N m kg 2 m The gravitational potential energy near the surface of a planet is equal to the product of the mass and the acceleration due to gravity and the vertical position of the object. Formula U g = m g y Units:Joules = kg m m= N m s 2

159 Mechanics The gravitational potential energy is equal quotient of the product of the universal gravitational constant the, mass of one object, mass of a secondobject and the distance between the objects Formula U g = G mm r Units Joules= 6.67x10 -11 N m 2 kg kg = N m kg 2 m The gravitational potential energy near the surface of a planet is equal to the product of the mass and the acceleration due to gravity and the vertical position of the object. Formula U g = m g y Units:Joules = kg m m= N m s 2

160 Mechanics The gravitational potential energy is equal quotient of the product of the universal gravitational constant the, mass of one object, mass of a secondobject and the distance between the objects Formula U g = G mm r Units Joules= 6.67x10 -11 N m 2 kg kg = N m kg 2 m The gravitational potential energy near the surface of a planet is equal to the product of the mass and the acceleration due to gravity and the vertical position of the object. Formula U g = m g y Units:Joules = kg m m= N m s 2

161 Mechanics Lab Experiences Run Out Back– time,distance, displacement, speed, velocity, acceleration are dependent on: measurements of: distance traveled or displacement, time elapsed v s = d v =  x a = v - v o t t t

162 Mechanics Labs-Graphical Analysis Vertical Jump Lab Cart up and Down Incline Position as a function of time graphs Velocity as a function of time graphs Acceleration as a function of time graphs x t V Constant,stopped a t t

163 Kinematic Equations - Projectiles Horizontal motion of a cart Vertical motion of dropped object Horizontally fired projectile v ox =v x =v o cos  Ground to ground fired projectile v oy =v o sin  X and Y positions as a function of time Y and X positions at maximum height Ground to cliff firing Cliff to ground firing

164 Kinematic Equations – Graphical and Analytic Solutions – Vector Quanitites Force Table X comp Y comp Sum of x Sum of y Resultant – Pythagorean theorem Tan y/x – Direction of resultant Tip to tail – Graphical analysis

165 Dynamics Fan Cart F=ma Cart Pulley Falling Mass m f g = a (m c + m f ) Block Pulley Falling Mass m f g -  m c g= a (m c + m f ) Cart on incline mgsin  = F parallel mgcos  =F perpendicular Block on Incline mgsin  =  mgcos  =F friction Stationary block on incline  mgcos  mgsin  Elevator lab-at rest, constant up, constant down accelerating up, coming to rest down accelerating down, coming to rest up Object 1 Pulley Heavier Object 2 m h g = a ( m h +m l ) Cart, Block on incline Pulley Falling Mass

166 Uniform Circular Motion Ball on String 2  r(rev) =v mv t Coin on Turntable Penny on Rotating Wall Car in hot wheel track Interactive Physics:  Earth Satellite  Earth Satellite Moon  Earth Geostationary Satellite Moon  Sun Earth Satellite Moon System  Bipolar Star System

167 Work / Energy / Power  U g mgy–mgy o  k = ½ mv 2- ½ mv o 2  U s = ½ kx 2 -½ kx o 2 Spring Cart Lab: E.P.E. to K.E. ½ kx 2 = ½ mv 2 Cart on Incline: G.P.E. to K.E. lab mg  y = ½ mv 2 Rollercoaster Interactive Physics: G.P.E. to K.E. lab Bow Lab : Work to E.P.E. to K.E. Force varies with distance = Work equals area under Force vs distance Power Lab: Wrist Roll, Sprint, Stair Climb P = mg  y P =  k = ½ mv 2- ½ mv o 2  t  t Electric Motor: P = IV and P output =  K.E +  G.P.E  t Trampoline Interactive Physics: G.P.E. to K.E to E.P.E – G.P.E

168 Conservation of Momentum Elastic Collision of light onto stationary heavy m L v oL = m L v L + m H v bounce back go forward p o =p k o =k Elastic Collision of heavy onto stationary light m H v oH = m H v H + m L v L both go forward p o =p k o =k Elastic Collision of heavy onto stationary heavy m H1 v oH1 = m H2 v H2 stop and go p o =p k o =k Elastic Head on Collisions of light onto light m L v oL1 + m L v oL2 = m L v L1 + m L v L2 switch p o =p k o =k Inelastic collision of light onto stationary heavy m L v oL = (m L + m H ) v LH Stick p o =p k o > k Inelastic collision of heavy onto stationary light m H v oH = (m H + m L ) v HL Stick p o =p k o >k

169 Conservation of Momentum Off center Collisions p ox = p x and p oy = p y If you start with only x momentum then any y momentum generated in one particle must be cancelled by the y momentum of another particle. Ballistic Sled Momentum conservationenergy conservation mv ob = ( m b + m s )v bs ½ (m b + m s )v bs 2 =  (m b + m s )gd Ballistic Pendulum Momentum conservationenergy conservation mv ob = ( m b + m p )v bp ½ (m b + m p )v bp 2 = (m b + m s )g  y

170 Impulse Change in Momentum Stiff Spring Soft Spring Rubber Bumper Magnetic bumper Force as a function of time graph analysis Rocket Thrust Analysis Newton's Third Law Connection to Change in momentum F t t Impulse = J = F  t =Change in momentum in N s = Area under the curve t t

171 Torque Interactive Physics Force applied at different distances from the center of rotation Force applied at different angles Clockwise and Counterclockwise Torque Problems ?

172 Moment of Inertia – Rotational Inertia Momentum of Inertia Demonstrations with rotating disk and rotating loop on an incline Balancing objects that are close to the center of rotation Balancing objects further from the center of rotation

173 Periodic Motion Simple harmonic motion of springs – interactive physics Simple harmonic motion of pendulums – Interactive physics Tp = 2  l T s = 2  m g k

174 Fluid Dynamics Pressure Pascals Principle Bouyant force

175 Fluids Can be Liquids Gases Because they can Flow

176 Fluids Can be Liquids Gases Because they can Flow

177 Fluids Can be Liquids Gases Because they can Flow

178 Fluids Can be Liquids Gases Because they can Flow

179 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

180 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

181 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

182 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

183 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

184 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

185 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

186 Fluid Pressure Scalar quantity Force acting perpendicular to and distributed over a surface, divided by the area of that surface P= F A

187 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

188 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

189 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

190 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

191 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

192 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

193 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

194 Scalar Pressure Pressure has magnitude but no Direction. The force exerted by a fluid at rest is always perpendicular to that surface P = F = Pascals = N = kg m = kg A m 2 m 2 s 2 m s 2

195 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg =  V g =  Ah g =  gh A A A A P =  gh

196 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg =  V g =  Ah g =  gh A A A A P =  gh

197 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg =  V g =  Ah g =  gh A A A A P =  gh

198 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg =  V g =  Ah g =  gh A A A A P =  gh

199 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg =  V g =  Ah g =  gh A A A A P =  gh

200 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = m  g h = m gh =  gh A A A h V P =  gh

201 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh  V g =  Ah g =  gh A A Ah A P =  gh

202 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh  V g =  Ah g =  gh A A Ah A P =  gh

203 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh = m gh =  gh = A A Ah V P =  gh

204 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh = m gh =  gh = A A Ah V P =  gh

205 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh = m gh =  gh A A Ah V P =  gh

206 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh = m gh =  gh A A Ah V P guage =  gh

207 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh = m gh =  gh A A Ah V P guage =  gh P absolute = P oatmosphere +  gh

208 Gravity and Pressure Fg = mg  m V V = Ah (for a cylinder) P= F = mg = mgh = m gh =  gh A A Ah V P guage =  gh P absolute = P o(atmosphere) +  gh

209 Pressure In a Container The pressure at every point at a given horizontal level in a single body of fluid at rest is the same. _____ pressure _____ pressure

210 Pressure In a Container The pressure at every point at a given horizontal level in a single body of fluid at rest is the same. Low pressure High pressure

211 Pressure In a Container The pressure at every point at a given horizontal level in a single body of fluid at rest is the same. Low pressure High pressure

212 Pressure In a Container The pressure at every point at a given horizontal level in a single body of fluid at rest is the same. Low pressure High pressure

213 Pascals Principle An external pressure applied to a fluid confined within a closed container is transmitted… undiminished throughout the entire fluid

214 Pascals Principle An external pressure applied to a fluid confined within a closed container is transmitted… undiminished throughout the entire fluid

215 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

216 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

217 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

218 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

219 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

220 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

221 Hydraulic Lifts F o = F Force output = Force input A o A Area output Area input large output force = small input force large output area = small input area A o =y (y=piston displacement) A y o

222 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

223 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

224 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

225 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

226 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

227 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

228 Bouyancy P = F A F B = A P 2 – A P 1 F B = A(  gh) h= height of the object F B =  gAh =  gV

229 Bouyancy F B =  gAh =  gV F B =  Vg = m V g V F B = mg =weight of fluid displaced An object immersed in a fluid will be lighter (buoyed up) by an amount equal to the weight of the fluid it displaces.

230 Bouyancy F B =  gAh =  gV F B =  Vg = m V g V F B = mg =weight of fluid displaced An object immersed in a fluid will be lighter (buoyed up) by an amount equal to the weight of the fluid it displaces.

231 Bouyancy F B =  gAh =  gV F B =  Vg = m V g V F B = mg =weight of fluid displaced An object immersed in a fluid will be lighter (buoyed up) by an amount equal to the weight of the fluid it displaces.

232 Bouyancy F B =  gAh =  gV F B =  Vg = m V g V F B = mg =weight of fluid displaced An object immersed in a fluid will be lighter (buoyed up) by an amount equal to the weight of the fluid it displaces.

233 Streamline Flow Characterized by ________path Path called a________ Streamlines ________cross

234 Equation of Continuity

235 Volume in

236 Equation of Continuity Volume in Volume out Volume in = Rate In = Rate Out = Volume out time time A 1 h 2 t A 2 h 2 t A 1 v 1 A 2 v 2

237 Equation of Continuity A 1 v 1 = A 2 v 2 The product of any cross-sectional area of the pipe and the fluid speed at that cross-section is constant. Conservation of matter.

238 Equation of Continuity A 1 v 1 = A 2 v 2 The product of any cross-sectional area of the pipe and the fluid speed at that cross-section is constant. Conservation of matter.

239 Equation of Continuity A 1 v 1 = A 2 v 2 The product of any cross-sectional area of the pipe and the fluid speed at that cross-section is constant. Conservation of matter.

240 Equation of Continuity A 1 v 1 = A 2 v 2 The condition Av = a constant is equivalent to the fact that the amount of fluid that enters one end of the tube in a given time interval ________ the amount of fluid leaving the tube in the same interval assuming the absence of leaks.

241 Equation of Continuity A 1 v 1 = A 2 v 2 The condition Av = a constant is equivalent to the fact that the amount of fluid that enters one end of the tube in a given time interval equals the amount of fluid leaving the tube in the same interval assuming the absence of leaks.

242 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related ________and ________to Fluid pressure It is an equation based on the Conservation of________

243 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related Fluid speed and elevation to fluid pressure It is an equation based on the conservation of energy

244 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related Fluid speed and elevation to fluid pressure It is an equation based on the conservation of energy

245 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related Fluid speed and elevation to fluid pressure It is an equation based on the conservation of energy

246 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related Fluid speed and elevation to fluid pressure It is an equation based on the conservation of energy

247 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related Fluid speed and elevation to fluid pressure It is an equation based on the conservation of energy

248 Bernoulli's Equation 1738 Daniel Bernoulli derived an equation that related Fluid speed and elevation to fluid pressure It is an equation based on the conservation of energy

249 Bernoulli's Equation Elevated Large cross sectional area Small cross sectional area

250 Bernoulli's Equation P = V = W 1 = W 2 =

251 Bernoulli's Equation P = F A V = W 1 = W 2 =

252 Bernoulli's Equation P = F A V = Ah W 1 = W 2 =

253 Bernoulli's Equation P = F A V = Ah W 1 = F 1 h = P 1 A 1 h 1 = P 1 V W 2 =

254 Bernoulli's Equation P = F A V = Ah W 1 = F 1 h = P 1 A 1 h 1 = P 1 V W 2 = F 2 h 2 = P 2 A 2 h 2 = P 2 V

255 Bernoulli's Equation W 2 = W = Work goes into changing the gravitational potential energy and part goes into changing the kinetic energy

256 Bernoulli's Equation W 2 = F 2 h 2 = P 2 A 2 h 2 = P 2 V W = Work goes into changing the gravitational potential energy and part goes into changing the kinetic energy

257 Bernoulli's Equation W 2 = F 2 h 2 = P 2 A 2 h 2 = P 2 V W = P 1 V – P 2 V Work goes into changing the gravitational potential energy and part goes into changing the kinetic energy

258 Bernoulli's Equation P 1 V – P 2 V = ½ mv 2 2 – ½ mv 1 2 + mgy 2 – mgy 1 Divide each term by ________to get P 1 – P 2 = ½  v 2 2 – ½  v 1 2 +  gy 2 –  gy 1

259 Bernoulli's Equation P 1 V – P 2 V = ½ mv 2 2 – ½ mv 1 2 + mgy 2 – mgy 1 Divide each term by Volume to get P 1 – P 2 = ½  v 2 2 – ½  v 1 2 +  gy 2 –  gy 1

260 Bernoulli's Equation Change in K.E = ½ mv 2 2 – ½ mv 1 2 Change in G.P.E = mgy 2 – mgy 1 Work = P 1 V – P 2 V P 1 V – P 2 V = ½ mv 2 2 – ½ mv 1 2 + mgy 2 – mgy 1

261 Bernoulli's Equation P 1 – P 2 = ½  v 2 2 – ½  v 1 2 +  gy 2 –  gy 1 Move small cross sectional terms to the ________side and large cross sectional terms to the ________side P 1 + ½  v 1 2 +  gy 1 = P 2 + ½  v 2 2 +  gy 2 P + ½  v 2 +  gy = Constant

262 Bernoulli's Equation P 1 – P 2 = ½  v 2 2 – ½  v 1 2 +  gy 2 –  gy 1 Move small cross sectional terms to the left side and large cross sectional terms to the right side P 1 + ½  v 1 2 +  gy 1 = P 2 + ½  v 2 2 +  gy 2 P + ½  v 2 +  gy = Constant

263 Bernoulli's Equation P + ½  v 2 +  gy = Constant The sum of the pressure, the kinetic energy per unit volume and the potential energy per unit volume has the ________value at all points along a streamline

264 Bernoulli's Equation P + ½  v 2 +  gy = Constant The sum of the pressure, the kinetic energy per unit volume and the potential energy per unit volume has the same value at all points along a streamline

265 Bernoulli's Equation P 1 + ½  v 1 2 +  gy 1 = P 2 + ½  v 2 2 +  gy 2 ________ pipe P 1 + ½  v 1 2 = P 2 + ½  v 2 2 Swiftly moving fluids exert _____ pressure than do slowly moving fluids

266 Bernoulli's Equation P 1 + ½  v 1 2 +  gy 1 = P 2 + ½  v 2 2 +  gy 2 Level pipe P 1 + ½  v 1 2 = P 2 + ½  v 2 2 Swiftly moving fluids exert less pressure than do slowly moving fluids

267 Bernoulli's Equation P 1 + ½  v 1 2 +  gy 1 = P 2 + ½  v 2 2 +  gy 2 Level pipe P 1 + ½  v 1 2 = P 2 + ½  v 2 2 Swiftly moving fluids exert less pressure than do slowly moving fluids

268 labs Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph = speed /velocity  Slope analysis of velocity as a function of time graph =acceleration  Area analysis of velocity as a function of time = displacement

269 labs Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph = speed /velocity  Slope analysis of velocity as a function of time graph =acceleration  Area analysis of velocity as a function of time = displacement

270 labs Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph = speed /velocity  Slope analysis of velocity as a function of time graph =acceleration  Area analysis of velocity as a function of time = displacement

271 labs Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph = speed /velocity  Slope analysis of velocity as a function of time graph =acceleration  Area analysis of velocity as a function of time = displacement

272 labs Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph = speed /velocity  Slope analysis of velocity as a function of time graph =acceleration  Area analysis of velocity as a function of time = displacement

273 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

274 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

275 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

276 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

277 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

278 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

279 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

280 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

281 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

282 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

283 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

284 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

285 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

286 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

287 Labs – kinematics in 1 and 2 dimensions Physics Terms Walking speed Walking Velocity Graphical Analysis  Slope analysis of position as a function of time graph  Slope analysis of velocity as a function of time graph  Area analysis of velocity as a function of time graph Analysis of a Vertical Jump Kinematics Equation analysis of cart up and down incline a=v-v o v =v +v o v= v o + at x=x o +v o t+ 1/2 at 2 v 2 =v o 2 +2a  x t 2 Free fall picket fence lab y vs t graph, v y vs t graph, and g vs t graph

288 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

289 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

290 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

291 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

292 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

293 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

294 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

295 Labs – kinematics in 1 and 2 dimensions Horizontally fired projectile  Time of flight is independent of horizontal velocity  Time of flight is dependent on height fired from Horizontal range as a function of angle for ground to ground fired projectiles  v ox =v o cos   v ox = v x  v oy = v o sin   v y = v oy + gt X and Y position as a function of time for a projectile fired at angle above or below the horizon X and Y position at maximum height for a projectile fired at an angle above the horizon ground to cliff fired projectiles cliff to ground fired projectiles  Quadratic equation to find time of flight y=y o + v oy t + ½ gt 2

296 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

297 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

298 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

299 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

300 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

301 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

302 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

303 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

304 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

305 Labs - force Force Table –  Graphical Method – tip to tail sketches  Analytical Method – Draw vectors from original Determine angles with respect to x axis Determine x components Determine y components Determine sum of x components Determine sum of y components Use Pythagorean Theorem to determine Resultant Force Use inv tan of sum of y components divided by sum of x components to determine angle with respect to x axis

306 Labs - Force Fan Cart F=ma Frictionless Cart pulled by falling mass fromula=a= m f g (m f +m c ) Friction Block pulled by falling mass formula = a = m f g –  mg ( m f + m b )

307 Labs - Force Fan Cart F=ma Frictionless Cart pulled by falling mass fromula= a= m f g (m f +m c ) Friction Block pulled by falling mass formula = a = m f g –  mg ( m f + m b )

308 Labs - Force Fan Cart F=ma Frictionless Cart pulled by falling mass fromula= a= m f g (m f +m c ) Friction Block pulled by falling mass formula = a = m f g –  m b g ( m f + m b )

309 Labs - Force Frictionless Cart on incline  Formula: a = gsin  Friction Block on incline  Formula: a = g sin  –  g cos  Friction Block on incline falling mass  Formula a = m f g - m b g cos  –  m b g sin   ( m f + m b )

310 Labs - Force Frictionless Cart on incline  Formula: a = gsin  Friction Block on incline  Formula: a = g sin  –  g cos  Friction Block on incline falling mass  Formula a = m f g - m b g cos  –  m b g sin   ( m f + m b )

311 Labs - Force Frictionless Cart on incline  Formula: a = gsin  Friction Block on incline  Formula: a = g sin  –  g cos  Friction Block on incline falling mass  Formula a = m f g - m b g cos  –  m b g sin   ( m f + m b )

312 Labs - Force Frictionless Cart on incline  Formula: a = gsin  Friction Block on incline  Formula: a = g sin  –  g cos  Friction Block on incline falling mass  Formula a = m f g - m b g sin  m b g cos   ( m f + m b )

313 Labs - Force Elevator lab – stationary, accelerating up, constant velocity up, decelerating up, stationary, accelerating down, constant velocity down, decelerating down, stationary, free fall Stationary, Constant Up, Constant Down Formula: F N = F g Accelerating up or Decelerating Down Formula: F N = F g + F net Accelerating down or Decelerating Up Formula: F N = F g - F net Freefall Formula: F N =0

314 Labs - Force Elevator lab – stationary, accelerating up, constant velocity up, decelerating up, stationary, accelerating down, constant velocity down, decelerating down, stationary, free fall Stationary, Constant Up, Constant Down Formula: F N = F g Accelerating up or Decelerating Down Formula: F N = F g + F net Accelerating down or Decelerating Up Formula: F N = F g - F net Freefall Formula: F N =0

315 Labs - Force Elevator lab – stationary, accelerating up, constant velocity up, decelerating up, stationary, accelerating down, constant velocity down, decelerating down, stationary, free fall Stationary, Constant Up, Constant Down Formula: F N = F g Accelerating up or Decelerating Down Formula: F N = F g + F net Accelerating down or Decelerating Up Formula: F N = F g - F net Freefall Formula: F N =0

316 Labs - Force Elevator lab – stationary, accelerating up, constant velocity up, decelerating up, stationary, accelerating down, constant velocity down, decelerating down, stationary, free fall Stationary, Constant Up, Constant Down Formula: F N = F g Accelerating up or Decelerating Down Formula: F N = F g + F net Accelerating down or Decelerating Up Formula: F N = F g - F net Freefall Formula: F N =0

317 Labs - Force Elevator lab – stationary, accelerating up, constant velocity up, decelerating up, stationary, accelerating down, constant velocity down, decelerating down, stationary, free fall Stationary, Constant Up, Constant Down Formula: F N = F g Accelerating up or Decelerating Down Formula: F N = F g + F net Accelerating down or Decelerating Up Formula: F N = F g - F net Freefall Formula: F N =0

318 Concept Maps Newtons three laws  Law of inertia Mass is a measure of inertia Object at rest stay at rest until net force acts on them Objects in with a constant speed moving in a straight line remain in this state until a net force acts on them

319 Concept Maps Newtons three laws  Law of inertia Mass is a measure of inertia Object at rest stay at rest until net force acts on them Objects in with a constant speed moving in a straight line remain in this state until a net force acts on them

320 Concept Maps Newtons three laws  Law of inertia Mass is a measure of inertia Object at rest stay at rest until net force acts on them Objects in with a constant speed moving in a straight line remain in this state until a net force acts on them

321 Concept Maps Newtons three laws  Law of inertia Mass is a measure of inertia Object at rest stay at rest until net force acts on them Objects in with a constant speed moving in a straight line remain in this state until a net force acts on them

322 Force concept maps Quantitative Second Law Force is equal to the change in momentum per unit of time Force is equal to the product of mass and acceleration

323 Force concept maps Quantitative Second Law Force is equal to the change in momentum per unit of time Force is equal to the product of mass and acceleration

324 Force concept maps Quantitative Second Law Force is equal to the change in momentum per unit of time Force is equal to the product of mass and acceleration

325 Force concept maps Quantitative Second Law Force is equal to the change in momentum per unit of time Force is equal to the product of mass and acceleration

326 Force concept maps Quantitative Second Law Force is equal to the change in momentum per unit of time Force is equal to the product of mass and acceleration

327 Force concept maps Action Reaction Third Law  Equal magnitude forces  Acting in opposite directions  Acting on two objects  Acting with the same type of force

328 Force concept maps Action Reaction Third Law  Equal magnitude forces  Acting in opposite directions  Acting on two objects  Acting with the same type of force

329 Force concept maps Action Reaction Third Law  Equal magnitude forces  Acting in opposite directions  Acting on two objects  Acting with the same type of force

330 Force concept maps Action Reaction Third Law  Equal magnitude forces  Acting in opposite directions  Acting on two objects  Acting with the same type of force

331 Force concept maps Action Reaction Third Law  Equal magnitude forces  Acting in opposite directions  Acting on two objects  Acting with the same type of force

332 Force concept maps Non contact forces  Force due to gravity  Electrostatic and Magnostatic forces  Strong and Weak nuclear force

333 Force concept maps Non contact forces  Force due to gravity  Electrostatic and Magnostatic forces  Strong and Weak nuclear force

334 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

335 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

336 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

337 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

338 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

339 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

340 Force concept maps Contact forces  Push – Normal Force – Perpendicular to a surface  Friction – requires normal force – opposes motion  Pull – Tension – acts in both directions

341 Free body diagrams  F g = force due to gravity = weight  F N = perpendicular push  F fr = opposes motion  F T = pull = tension

342 Free body diagrams  F g = force due to gravity = weight  F N = perpendicular push  F fr = opposes motion  F T = pull = tension

343 Free body diagrams  F g = force due to gravity = weight  F N = perpendicular push  F fr = opposes motion  F T = pull = tension

344 Free body diagrams  F g = force due to gravity = weight  F N = perpendicular push  F fr = opposes motion  F T = pull = tension

345 Free body diagrams  F g = force due to gravity = weight  F N = perpendicular push  F fr = opposes motion  F T = pull = tension

346 Labs – Uniform Circular Motion Swing ride – Tension creates a center seeking force – centripetal force Gravitron- Normal force creates a center seeking force – centripetal force Hotwheel rollercoaster – Weightlessness at top – gravity creates the center seeking force – centripetal force Turntable ride – friction creates a central seeking force – centripetal force

347 Labs – Uniform Circular Motion Swing ride – Tension creates a center seeking force – centripetal force Gravitron- Normal force creates a center seeking force – centripetal force Hotwheel rollercoaster – Weightlessness at top – gravity creates the center seeking force – centripetal force Turntable ride – friction creates a central seeking force – centripetal force

348 Labs – Uniform Circular Motion Swing ride – Tension creates a center seeking force – centripetal force Gravitron- Normal force creates a center seeking force – centripetal force Hotwheel rollercoaster – Weightlessness at top – gravity creates the center seeking force – centripetal force Turntable ride – friction creates a central seeking force – centripetal force

349 Labs – Uniform Circular Motion Swing ride – Tension creates a center seeking force – centripetal force Gravitron- Normal force creates a center seeking force – centripetal force Hotwheel rollercoaster – Weightlessness at top – gravity creates the center seeking force – centripetal force Turntable ride – friction creates a central seeking force – centripetal force

350 Labs – Uniform Circular Motion Swing ride – Tension creates a center seeking force – centripetal force Gravitron- Normal force creates a center seeking force – centripetal force Hotwheel rollercoaster – Weightlessness at top – gravity creates the center seeking force – centripetal force Turntable ride – friction creates a central seeking force – centripetal force

351 Labs – Uniform Circular Motion Swing ride – Tension creates a center seeking force – centripetal force Gravitron- Normal force creates a center seeking force – centripetal force Hotwheel rollercoaster – Weightlessness at top – gravity creates the center seeking force – centripetal force Turntable ride – friction creates a central seeking force – centripetal force

352 Labs – Uniform Circular Motion Cavendish Torsion Balance – F g = G m 1 m 2 r 2 Universal Gravitational Constant – big G = 6.67x10 -11 Nm 2 /kg 2 Mass of the earth calculation mg = G m 1 m e r 2 Earth’s moon orbital velocity calculation Satellite orbital velocity calculation Geostationary Satellite orbital velocity and orbital radius calculation Bipolar Star calculation F c = mv 2 = G m 1 m 2 = F g v= 2  r(rev) r r 2 t

353 Labs – Uniform Circular Motion Cavendish Torsion Balance – F g = G m 1 m 2 r 2 Universal Gravitational Constant – big G = 6.67x10 -11 Nm 2 /kg 2 Mass of the earth calculation mg = G m 1 m e r 2 Earth’s moon orbital velocity calculation Satellite orbital velocity calculation Geostationary Satellite orbital velocity and orbital radius calculation Bipolar Star calculation F c = mv 2 = G m 1 m 2 = F g v= 2  r(rev) r r 2 t

354 Labs – Uniform Circular Motion Cavendish Torsion Balance – F g = G m 1 m 2 r 2 Universal Gravitational Constant – big G = 6.67x10 -11 Nm 2 /kg 2 Mass of the earth calculation mg = G m 1 m e r 2 Earth’s moon orbital velocity calculation Satellite orbital velocity calculation Geostationary Satellite orbital velocity and orbital radius calculation Bipolar Star calculation F c = mv 2 = G m 1 m 2 = F g v= 2  r(rev) r r 2 t

355 Labs – Uniform Circular Motion Cavendish Torsion Balance – F g = G m 1 m 2 r 2 Universal Gravitational Constant – big G = 6.67x10 -11 Nm 2 /kg 2 Mass of the earth calculation mg = G m 1 m e r 2 Earth’s moon orbital velocity calculation Satellite orbital velocity calculation Geostationary Satellite orbital velocity and orbital radius calculation Bipolar Star calculation F c = mv 2 = G m 1 m 2 = F g v= 2  r(rev) r r 2 t

356 Labs – Uniform Circular Motion Cavendish Torsion Balance – F g = G m 1 m 2 r 2 Universal Gravitational Constant – big G = 6.67x10 -11 Nm 2 /kg 2 Mass of the earth calculation mg = G m 1 m e r 2 Earth’s moon orbital velocity calculation Satellite orbital velocity calculation Geostationary Satellite orbital velocity and orbital radius calculation Bipolar Star calculation F c = mv 2 = G m 1 m 2 = F g v= 2  r(rev) r r 2 t

357 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

358 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

359 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

360 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

361 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

362 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

363 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

364 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

365 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity

366 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration

367 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum

368 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum

369 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum (Change)

370 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum (Change) Force

371 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force

372 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force

373 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force

374 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force Work /

375 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force Work / Energy

376 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force Work / Energy

377 Kinematics / Dynamics Relationships Distance / Displacement Time Mass Speed/Velocity acceleration Momentum Force Work / Energy Power

378 Kinematics / Dynamics Relationships Distance/DisplacementTimeMass m/s

379 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s m/s/s=m/s 2

380 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity = m/s Acceleration =m/s 2

381 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s kg m/s Acceleration= m/s 2

382 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s kg m/s-momentum Acceleration= m/s 2

383 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 kg m/s/s=kg m/s 2

384 Kinematics / Dynamics Relationships Distance/DisplacementTimeMass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=Newton=kg m/s 2

385 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 kg m/s 2

386 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=Newton =kg m/s 2

387 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force= Newtons=kg m/s 2 N m = Kg m/s 2 m

388 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=Newtons = kg m/s 2 N m = Kg m 2 /s 2

389 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=Newton=kg m/s 2 Work /

390 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=Newton=kg m/s 2 Work / Energy = Joule = N m = kg m 2 /s 2

391 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=N=kg m/s 2 Work / Energy=J = N m = kg m 2 / s 2 kg m 2 /s 2 /s

392 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=N=kg m/s 2 Work / Energy=J = N m = kg m 2 / s 2 kg m 2 /s 2 /s = kg m 2 /s 3

393 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=N=kg m/s 2 Work / Energy=J = N m = kg m 2 / s 2 kg m 2 /s 2 /s = kg m 2 /s 3 = N m = J s s

394 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=N=kg m/s 2 Work / Energy=J = N m = kg m 2 / s 2 kg m 2 /s 2 /s = kg m 2 /s 3 = N m = J = W s s

395 Kinematics / Dynamics Relationships Distance/DisplacementTime Mass Speed/Velocity=m/s Momentum=kg m/s Acceleration=m/s 2 Force=N=kg m/s 2 Work / Energy=J = N m = kg m 2 / s 2 Power kg m 2 /s 2 /s = kg m 2 /s 3 = N m = J = W s s

396 Graphical Analysis Position Time

397 Graphical Analysis Position Time

398 Graphical Analysis Position Time

399 stopped Position Time

400 Graphical Analysis Position Time

401 Constant velocity –constant momentum – no acceleration Position Time

402 Graphical Analysis Position Time

403 Constant velocity – constant momentum – no acceleration Position Time

404 Graphical Analysis Position Time

405 Increasing velocity – increasing momentum - accelerating Position Time

406 Graphical Analysis Position Time

407 Increasing velocity – increasing momentum - accelerating Position Time

408 Graphical Analysis Position Time

409 Decreasing velocity – decreasing momentum - decelerating Position Time

410 Graphical Analysis Position Time

411 Decreasing velocity – decreasing momentum - decelerating Position Time

412 Graphical Analysis O m/s

413 Velocity vs Time Velocity 0 m/s time

414 O m/s

415 Stopped O m/s

416

417 Accelerating O m/s

418

419 accelerating O m/s

420 decelerating O m/s

421 decelerating O m/s

422 decelerating O m/s

423 decelerating O m/s

424

425 Constant velocity O m/s

426

427 Constant Velocity O m/s

428 Graphical Analysis Slopes Postion time

429 Slope = velocity Postion time

430 Velocity vs Time Slope Velocity time

431 Slope of V vs T = Acceleration Velocity time

432 Area of V vs T = ? Velocity time

433 Area of V vs T = Distance traveled Velocity time

434 Area of V vs T = Distance traveled Velocity time

435 Force vs Distance Force Distance

436 Force vs Distance Force slope = spring constant K = N m Distance

437 Force vs Distance Force E.P.E=1/2 Kx 2 Distance

438 Force vs Distance Force Area = Work Distance

439 Force vs time Force Time

440 Force vs time Area Force Change in Momentum = Time

441 Force vs time Area Force Change in Momentum =  p = J Impulse = Average Force * time J = F avg t = N*s Time


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