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PHY 101: Lecture 8 8.1 Rotational Motion and Angular Displacement 8.2 Angular Velocity and Angular Acceleration 8.3 The Equations of Rotational Kinematics.

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Presentation on theme: "PHY 101: Lecture 8 8.1 Rotational Motion and Angular Displacement 8.2 Angular Velocity and Angular Acceleration 8.3 The Equations of Rotational Kinematics."— Presentation transcript:

1 PHY 101: Lecture 8 8.1 Rotational Motion and Angular Displacement 8.2 Angular Velocity and Angular Acceleration 8.3 The Equations of Rotational Kinematics 8.4 Angular Variables and Tangential Variables 8.5 Centripetal Acceleration and Tangential Acceleration 8.6 Rolling Motion 8.7 Vector Nature of Angular Variables

2 PHY 101: Lecture 8 Rotational Kinematics 8.1 Rotational Motion and Angular Displacement

3 Rotational Motion and Angular Displacement - 1 In the simplest kind of rotation, points on a rigid object move on circular paths –In the example, we see the circular paths for points A, B, and C –The center of all such circular paths define a line, called the axis of rotation

4 Rotational Motion and Angular Displacement - 2 The angle through which a rigid object rotates about a fixed axis is called the angular displacement –The figure shows how the angular displacement is measured for a rotating disc –The axis of rotation passes through the center of the disc and is perpendicular to the disc

5 Rotational Motion and Angular Displacement - 3 On the surface of the disc draw a radial line, which is a line that intersects the axis of rotation perpendicularly As the disc turns, we observe the angle through which this line moves relative to a convenient reference line that does not rotate The radial line moves from its initial orientation at an angle  0 to a final orientation at angle 

6 Rotational Motion and Angular Displacement - 4 The line sweeps out the angle  =  –  0 Counter clockwise displacement is positive Clockwise displacement is negative

7 Rotational Motion and Angular Displacement - 5 SI Unit of Angular Displacement: radian (rad) –Figure shows how the radian is defined –The figure focuses attention on a point P on the disc –Point P starts out on the stationary reference line so that  0 = 0 rad –Angular displacement is  =  –  0 = 

8 Rotational Motion and Angular Displacement - 6 –As the disc rotates, the point traces out an arc of length s, which is measured along a circle of radius r –The angle q in radian\  rad = Arc length / Radius = s/r

9 Rotational Motion and Angular Displacement - 7 To find number of radians in a full circle take circumference 2  r and divide by radius to get 2  radians To convert from degrees to radians  radians = degrees x (2  / 360) To convert from radians to degrees  degrees = radians x (360 / 2  )

10 Rotational Motion and Angular Displacement - 7 How many degrees is an angle of 1 radian? degrees = 1 radian x (360/2  ) = 57.3 0 1 radian is a large angle

11 Example 1 How many radians is an angle of 30 0 ?  radians = 30 0 x (2  /360) = 0.52 radians

12 Example 2 The bob of a pendulum that is 0.80 m long swings through an angle of 0.2 radians Find length of arc through which it swings  An angle of 1 radian has an arc length on the circle equal to the radius of the circle  If you take the arc length and divide by the radius, you get the number of radians  radians = 0.20 = d / 0.80 radius  d = 0.16 m

13 PHY 101: Lecture 8 Rotational Kinematics 8.2 Angular Velocity and Angular Acceleration

14 Angular Velocity

15 Angular Acceleration

16 PHY 101: Lecture 8 Rotational Kinematics 8.3 Equations of Rotational Kinematics

17 Equation of Rotational Kinematics

18 PHY 101: Lecture 8 Rotational Kinematics 8.4 Angular Variables and Tangential Variables

19 Relationship Linear and Circular Quantities  d = r   v = r   a = r  r is the radius of the circle d is the arc length of path around circle v is the speed tangent to the circle a is the acceleration tangent to the circle

20 Circular Motion Equations of Motion x = r(cos  y = r(sin   =  t x = r(cos  t)(Equation of motion) y = r(sin  t)(Equation of motion)

21 Linear and Circular Quantities Example 1 For a circle with a radius of 1 m, what is the arc length of an angle of 2 radians?  arc length = d = r   arc length = (1 m)(2 radians) = 2 m

22 Linear and Circular Quantities Example 2 An object travels around a circle with a radius of 1.4 m with a tangential velocity of 5 m/s What is the angular velocity?   = v/r   = (5 m/s) / 1.4 m = 3.57 radians/s

23 Circular Motion Descriptive Properties Period (T)  Time it takes to complete one cycle or one complete trip around the circle  SI Units are second/cycle Frequency (f)  Number of cycles per second  SI Units are cycles/second or Hertz (Hz)  f = 1/T Angular Frequency (  )  The number of radians per second  SI Units are radians/second   = 2  f

24 Circular Motion Descriptive Quantities – Example What is the (a) period and (b) angular frequency of an old-fashioned phonograph record that turns through 100 rotations per second?  A rotation per second is the same as cycles per second  Cycle per second is frequency, f = 100  The period T is 1/f = 1/100 = 0.01 s/cycle  The angular frequency or angular velocity is  = 2  f = 2  (100) = 628.3 rad/s


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