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Lecture 7 Newton’s Laws of Motion. Midterm Test #1 - Thursday!  21 multiple-choice problems - A calculator will be needed. - CHECK YOUR BATTERIES! -

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Presentation on theme: "Lecture 7 Newton’s Laws of Motion. Midterm Test #1 - Thursday!  21 multiple-choice problems - A calculator will be needed. - CHECK YOUR BATTERIES! -"— Presentation transcript:

1 Lecture 7 Newton’s Laws of Motion

2 Midterm Test #1 - Thursday!  21 multiple-choice problems - A calculator will be needed. - CHECK YOUR BATTERIES! - NO equations or information may be stored in your calculator. This is part of your pledge on the exam. - Scratch paper will be provided, to be turned in at the end of the exam.  A sign-in sheets will be used, photographs of the class will be taken, all test papers will be collected

3 F top F bot W A weight on a string... if I pull the bottom string down, which string will break first? a) top string b) bottom string c) there is not enough information to answer this question How quickly is the string pulled? A sudden, strong tug is resisted by the inertia of the mass, protecting the top string. A gradual pull forces the top string to keep the system in equilibrium.

4 Translation Equilibrium “translational equilibrium” = fancy term for not accelerating = the net force on an object is zero example: book on a table example: book on a table in an elevator at constant velocity

5 Before practicing his routine on the rings, a 67-kg gymnast stands motionless, with one hand grasping each ring and his feet touching the ground. Both arms slope upward at an angle of 24° above the horizontal. (a) If the force exerted by the rings on each arm has a magnitude of 290 N, and is directed along the length of the arm, what is the magnitude of the force exerted by the floor on his feet? (b) If the angle his arms make with the horizontal is greater that 24°, and everything else remains the same, is the force exerted by the floor on his feet greater than, less than, or the same as the value found in part (a)? Explain.

6 Before practicing his routine on the rings, a 67-kg gymnast stands motionless, with one hand grasping each ring and his feet touching the ground. Both arms slope upward at an angle of 24° above the horizontal. (a) If the force exerted by the rings on each arm has a magnitude of 290 N, and is directed along the length of the arm, what is the magnitude of the force exerted by the floor on his feet? (b) If the angle his arms make with the horizontal is greater that 24°, and everything else remains the same, is the force exerted by the floor on his feet greater than, less than, or the same as the value found in part (a)? Explain. N a) b) if the angle is larger and everything else remains the same, the applied forces are more vertical. With more upward force from the arms, LESS normal force is required for zero acceleration

7 Lecture 6 Applications of Newton’s Laws (Chapter 6)

8 8 a) N > mg b) N = mg c) N < mg (but not zero) d) N = 0 e) depends on the size of the elevator m a A block of mass m rests on the floor of an elevator that is accelerating upward. What is the relationship between the force due to gravity and the normal force on the block? Going Up II

9 9 The block is accelerating upward, so it must have a net upward force. The forces on it are N (up) and mg (down), so N must be greater than mg in order to give the net upward force! a) N > mg b) N = mg c) N < mg (but not zero) d) N = 0 e) depends on the size of the elevator  F = N – mg = ma > 0 Thus, N =mg+ma > mg m a > 0 mg N A block of mass m rests on the floor of an elevator that is accelerating upward. What is the relationship between the force due to gravity and the normal force on the block? Going Up II Follow-up: What is the normal force if the elevator is in free fall downward?

10 10 You are holding your 2.0 kg physics text book while standing on an elevator. Strangely, the book feels as if it weighs exactly 2.5 kg. From this, you conclude that the elevator is: Elevate Me a) in freefall b) moving upwards with a constant velocity of 4.9 m/s c) moving down with a constant velocity of 4.9 m/s d) experiencing a constant acceleration of about 2.5 m/s 2 upward e) experiencing a constant acceleration of about 2.5 m/s 2 downward 10

11 Use Newton’s 2 nd law! the apparent weight: You are holding your 2.0 kg physics text book while standing on an elevator. Strangely, the book feels as if it weighs exactly 2.5 kg. From this, you conclude that the elevator is: Elevate Me a) in freefall b) moving upwards with a constant velocity of 4.9 m/s c) moving down with a constant velocity of 4.9 m/s d) experiencing a constant acceleration of about 2.5 m/s 2 upward e) experiencing a constant acceleration of about 2.5 m/s 2 downward and the sum of forces: give a positive acceleration a y

12 12 Frictional Forces Friction has its basis in surfaces that are not completely smooth:

13 Kinetic friction Kinetic friction: the friction experienced by surfaces sliding against one another The frictional force is proportional to the contact force between the two surfaces (normal force): The constant is called the coefficient of kinetic friction. f k always points in the direction opposing motion of two surfaces

14 Frictional Forces fkfk fkfk Naturally, for any frictional force on a body, there is an opposing reaction force on the other body

15 Frictional Forces fkfk fkfk when moving, one bumps “skip” over each other fsfs fsfs when relative motion stops, surfaces settle into one another static friction

16 The static frictional force tries to keep an object from starting to move when other forces are applied. Static Friction The static frictional force has a maximum value, but may take on any value from zero to the maximum... depending on what is needed to keep the sum of forces to zero. The maximum static frictional force is also proportional to the contact force

17 A block sits on a flat table. What is the force of static friction? Static Friction a) zero b) infinite c) you need to tell me stuff, like the mass of the block, μ s, and what planet this is happening on

18 Characteristics of Frictional Forces Frictional forces always oppose relative motion Static and kinetic frictional forces are independent of the area of contact between objects Kinetic frictional force is also independent of the relative speed of the surfaces. (twice the mass = twice the weight = twice the normal force = twice the frictional force) Coefficients of friction are independent of the mass of objects, but in (most) cases forces are not:

19 Coefficients of Friction Q: what units?

20 20 Measuring static coefficient of friction N W fsfs   x y WxWx WyWy If the block doesn’t move, a=0. at the critical point Given the “critical angle” at which the block starts to slip, what is μ s ?

21 21 Acceleration of a block on an incline N W fkfk   x y WxWx WyWy If the object is sliding down - v

22 22 Acceleration of a block on an incline N W fkfk   x y WxWx WyWy If the object is sliding up - v What will happen when it stops?

23 23 m a) not move at all b) slide a bit, slow down, then stop c) accelerate down the incline d) slide down at constant speed e) slide up at constant speed A mass m is placed on an inclined plane (  > 0) and slides down the plane with constant speed. If a similar block (same  ) of mass 2m were placed on the same incline, it would: Sliding Down II

24 24 The component of gravity acting down the plane is double for 2m. However, the normal force (and hence the friction force) is also double (the same factor!). This means the two forces still cancel to give a net force of zero. A mass m is placed on an inclined plane (  > 0) and slides down the plane with constant speed. If a similar block (same  ) of mass 2m were placed on the same incline, it would:  W N f  WxWx WyWy a) not move at all b) slide a bit, slow down, then stop c) accelerate down the incline d) slide down at constant speed e) slide up at constant speed Sliding Down II

25 25 Tension When you pull on a string or rope, it becomes taut. We say that there is tension in the string. Note: strings are “floppy”, so force from a string is along the string!

26 26 Tension in a chain W T up T down T up = T down when W = 0 In this class: we will assume that all ropes, strings, wires, etc. are massless unless otherwise stated. Tension is the same everywhere in a massless rope!

27 27 Massive vs. Massless Rope The tension in a real rope will vary along its length, due to the weight of the rope. In this class: we will assume that all ropes, strings, wires, etc. are massless unless otherwise stated. T 1 = mg m T 3 = mg + W r T 2 = mg + W r /2 Tension is the same everywhere in a massless rope!

28 28 Three Blocks T3T3 T2T2 T1T1 3m3m 2m2m m a a) T 1 > T 2 > T 3 b) T 1 < T 2 < T 3 c) T 1 = T 2 = T 3 d) all tensions are zero e) tensions are random Three blocks of mass 3m, 2m, and m are connected by strings and pulled with constant acceleration a. What is the relationship between the tension in each of the strings?

29 29 T 1 pulls the whole set of blocks along, so it must be the largest. T 2 pulls the last two masses, but T 3 only pulls the last mass. Three Blocks T3T3 T2T2 T1T1 3m3m 2m2m m a a) T 1 > T 2 > T 3 b) T 1 < T 2 < T 3 c) T 1 = T 2 = T 3 d) all tensions are zero e) tensions are random Three blocks of mass 3m, 2m, and m are connected by strings and pulled with constant acceleration a. What is the relationship between the tension in each of the strings? Follow-up: What is T 1 in terms of m and a?

30 30 Tension Force is always along a rope W TT TyTy TT

31 31 Idealization: The Pulley An ideal pulley is one that simply changes the direction of the tension distance box moves = distance hands move speed of box = speed of hands acceleration of box = acceleration of hands

32 32 Tension in the rope?

33 33 2.00 kg Tension in the rope? W W T T

34 34 fkfk y : m 1 : x : m 2 : y : μkμk μkμk μkμk μkμk μkμk

35 35 Over the Edge m 10 kg a m a F = 98 N Case (1) Case (2) a) case (1) b) acceleration is zero c) both cases are the same d) depends on value of m e) case (2) In which case does block m experience a larger acceleration? In case (1) there is a 10 kg mass hanging from a rope and falling. In case (2) a hand is providing a constant downward force of 98 N. Assume massless rope and frictionless table. 35

36 36 In case (2) the tension is 98 N due to the hand. In case (1) the tension is less than 98 N because the block is accelerating down. Only if the block were at rest would the tension be equal to 98 N. Over the Edge m 10 kg a m a F = 98 N Case (1) Case (2) a) case (1) b) acceleration is zero c) both cases are the same d) depends on value of m e) case (2) In which case does block m experience a larger acceleration? In case (1) there is a 10 kg mass hanging from a rope and falling. In case (2) a hand is providing a constant downward force of 98 N. Assume massless rope and frictionless table. 36

37 37 Springs Hooke’s law for springs states that the force increases with the amount the spring is stretched or compressed: The constant k is called the spring constant.

38 38 Springs Note: we are discussing the force of the spring on the mass. The force of the spring on the wall are equal, and opposite.

39 39 Springs and Tension A mass M hangs on spring 1, stretching it length L 1 Mass M hangs on spring 2, stretching it length L 2 Now spring1 and spring2 are connected end-to-end, and M1 is hung below. How far does the combined spring stretch? S1S1 S2S2 a) (L 1 + L 2 ) / 2 b) L 1 or L 2, whichever is smaller c) L 1 or L 2, whichever is bigger d) depends on which order the springs are attached e) L 1 + L 2

40 40 Springs and Tension A mass M hangs on spring 1, stretching it length L 1 Mass M hangs on spring 2, stretching it length L 2 Now spring1 and spring2 are connected end-to-end, and M1 is hung below. How far does the combined spring stretch? S1S1 S2S2 W F s =T a) (L 1 + L 2 ) / 2 b) L 1 or L 2, whichever is smaller c) L 1 or L 2, whichever is bigger d) depends on which order the springs are attached e) L 1 + L 2

41 41 Springs and Tension A mass M hangs on spring 1, stretching it length L 1 Mass M hangs on spring 2, stretching it length L 2 Now spring1 and spring2 are connected end-to-end, and M1 is hung below. How far does the combined spring stretch? Spring 1 supports the weight. Spring 2 supports the weight. Both feel the same force, and stretch the same distance as before. S1S1 S2S2 W F s =T a) (L 1 + L 2 ) / 2 b) L 1 or L 2, whichever is smaller c) L 1 or L 2, whichever is bigger d) depends on which order the springs are attached e) L 1 + L 2


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