MR. SURRETTE VAN NUYS HIGH SCHOOL CHAPTER 6: ROTATION (PART 1) CLASS NOTES CIRCULAR MOTION Circular motion refers to the motion of a body about a fixed radius. One complete rotation about the center (360o) is called a revolution. RADIANS The fundamental unit of circular motion is the radian, commonly abbreviated rad or rads: One radian occurs when s = r. RADIANS CONVERSION The circumference of a circle is: C = 2r Therefore, for every complete turn along the circumference of a circle, we can trace out 2 radians. This leads to the following conversion: 2 radians = 1 revolution ANGULAR DISTANCE is the distance traveled in radians, it is an angular measurement. ANGULAR VELOCITY is the angular velocity, measured in rads/sec. TANGENTIAL VELOCITY Tangential velocity is the linear speed traveled by an object along the arc of a circle: v = r Note: The direction of the velocity vector is a tangent to the circular path. Example 1. A point on a wheel rotating at 5 rev/s and located 0.2 m from the axis has what tangential velocity? 1A. (1) = (5 rev/s)(2 rad/rev) = 31.4 rad/s (2) v = r (3) v = (0.2 m)(31.4 rad/s) (4) v = 6.3 m/s 1|Page PHYSICS MR. SURRETTE VAN NUYS HIGH SCHOOL ANGULAR ACCELERATION is the angular acceleration, measured in rads/s2. TANGENTIAL ACCELERATION Tangential acceleration is the linear acceleration along the arc of a circle: at = r CENTRIPETAL ACCELERATION In circular motion, the centripetal acceleration is directed inward toward the center of the circle: ac = v2/r Example 2. A point on the rim of a 0.20 m radius rotating wheel has a centripetal acceleration of 4.0 m/s2. What is the angular velocity of the wheel? 2A. (1) ac = v2/r (2) v2 = rac (3) v = (rac)1/2 (4) v = [(0.2 m)(4.0 m/s2)]1/2 (5) v = 0.89 m/s (6) v = r (7) = v/r (8) = 0.89 m/s / 0.20 m (9) = 4.47 rad/s Example 3. What angular velocity (in revs/sec) is needed for a centrifuge to produce an acceleration of 1000 g (1000 times the force of gravity) on a radius arm of 10 cm? 3A. (1) ac = v2/r (2) v2 = rac (3) v = (rac)1/2 (4) v = [(0.10 m)(1000)(9.8 m/s2)]1/2 (5) v = 31.3 m/s (6) v = r (7) = v/r (8) = (31.3 m/s)/(0.1 m) (9) = 313 rad/s (10) (313 rad / 1 sec)(1 rev / 2 rad) (11) = 49.8 rev/s CIRCULAR MOTION KINEMATICS Circular motion equations derive from linear motion equations: d (distance in meters) ~ (distance in radians) v (velocity in m/s) ~ (velocity in rads/s) 2 a (acceleration in m/s ) ~ (acceleration in rads/s2) 2|Page PHYSICS MR. SURRETTE VAN NUYS HIGH SCHOOL CIRCULAR MOTION EQUATIONS Circular Equation = ot + ½ t2 = o + t 2 = o2 + 2 Linear Equation (d = vot + ½ at2) (v = vo + at) (v2 = vo2 + 2ad) Example 4. A Ferris wheel, rotating initially at an angular velocity of 0.50 rad/s, accelerates over a 5 s interval at a rate of 0.04 rad/s2. What angular displacement does the Ferris wheel undergo in this 5 s interval? 4A. (1) = ot + ½ t2 (2) = (0.50 rad/s)(5 s) + ½ (0.04 rad/s2)(5 s)2 (3) = 3.0 rad Example 5. A Ferris wheel, starting at rest, builds up to a final angular velocity of 0.71 rad/s while rotating through an angular displacement of 2.5 rad. What is its average angular acceleration? 5A. (1) 2 = o2 + 2 (2) 2 = 0 + 2 (3) 2 = 2 (4) = 2 / 2 (5) = (0.71 rad/s)2 / 2(2.5 rad) (6) = 0.10 rad/s2 CENTRIPETAL FORCE All centripetal forces act toward the center of the circular path along which the object moves: Fc = mv2/r Example 6. A 0.3 kg mass, attached to the end of a 0.75 m string, is whirled around in a circular horizontal path. If the maximum tension that the string can withstand is 250 N, then what maximum velocity can the mass have if the string is not to break? 6A. (1) Fc = mv2/r (2) v2 = rFc/m (3) v = (rFc/m)1/2 (4) v = [(0.75 m)(250 N)/(0.3 kg)]1/2 (5) v = 25.0 m/s 3|Page PHYSICS MR. SURRETTE VAN NUYS HIGH SCHOOL Example 7. A roller coaster, loaded with passengers, has a mass of 500 kg; the radius of curvature of the track at the bottom point of the dip is 12 m. If the vehicle has a speed of 18 m/s at this point, what force is exerted on the vehicle by the track? 7A. (1) The track must support the weight of the coaster and the centripetal force of its motion: (2) Track = weight + Fc (3) Track = mg + mv2/r (4) (500 kg)(9.8 m/s2) + [(500 kg)(18 m/s)2] / 12 m (5) Track = 4900 N + 13,500 N (6) Track = 1.84 x 104 N Example 8. A car rounds a circular turn of radius r = 80 m in a horizontal (unbanked) road. A rear view of the car is given below. The coefficient of static friction between tires and road is 0.65 (we assume static friction because we don’t want the car to slide (that is skid)). The car’s weight mg is 1.2 x 104 N. Example 8. 8a. A. (1) (2) (3) (4) (5) (6) (7) What is the magnitude of the static force of friction when the car’s speed v = 20 m/s? Fc = mv2/r w = mg m = w/g m = (1.2 x 104 N) / (9.8 m/s2) m = 1224 kg Fc = (1224 kg)(20 m/s)2 / (80 m) Fc = 6120 N 8b. What is the maximum value of the static frictional force? A. (1) Fc (max): fs = n (2) fs = w (3) fs = (0.65)(1.2 x 104 N) (4) fs = 7800 N 4|Page PHYSICS MR. SURRETTE 8c. A. (1) (2) (3) (4) (5) (6) VAN NUYS HIGH SCHOOL Determine the maximum speed for the car to make it around the curve. Fc = mv2/r mv2 = rFc v2 = (rFc) / m v = (rFc /m)1/2 v = [(80 m)(7800 N) / (1224 kg)]1/2 v = 22.6 m/s 5|Page PHYSICS