CHAPTER 17 MOTION IN A CIRCLE EXERCISE 90, Page 199 1. A locomotive travels around a curve of 500 m radius. If the horizontal thrust on the outer rail is 1 of the locomotive weight, determine the speed of the locomotive. The surface that the rails 50 are on may be assumed to be horizontal and the horizontal force on the inner rail may be assumed to be zero. Centrifugal force on outer rail = mg 50 mv 2 mg = 50 r Hence, v2 = from which, i.e. v= gr 9.81 500 = = 98.1 m 2 /s 2 50 50 98.1 = 9.9 m/s = 9.9 m 1km 3600s s 1000 m 1h i.e. the speed of the locomotive, v = 35.64 km/h 2. If the horizontal thrust on the outer rail of Problem 1 is 1 of the locomotive’s weight, 100 determine its speed. Centrifugal force on outer rail = Hence, from which, i.e. mg 100 mv 2 mg = 100 r v2 = v= gr 9.81 500 = = 49.05 m 2 /s 2 100 100 49.05 = 7 m/s 225 © John Bird & Carl Ross Published by Taylor and Francis = (7 3.6) km/h i.e. the speed of the locomotive, v = 25.2 km/h 3. What angle of banking of the rails of Problem 1 is required for the outer rail to have a zero value of outward thrust? Assume the speed of the locomotive is 15 km/h. v2 Angle of banking, = tan 1 rg v = 15 km/h = 15 15 km 1h 1000 m = = 4.1667 m/s 3.6 h 3600s 1km 4.1667 2 m 2 / s 2 Hence, = tan = tan 1 (0.0035395) 2 500 m 9.81m / s 1 i.e. angle of banking, = 0.203 4. What angle of banking of the rails is required for Problem 3, if the speed of the locomotive is 30 km/h ? v2 Angle of banking, = tan 1 rg v = 30 km/h = 30 30 km 1h 1000 m = = 8.3333 m/s 3.6 h 3600s 1km 8.33332 m 2 / s 2 Hence, = tan = tan 1 (0.014158) 2 500 m 9.81m / s 1 i.e. angle of banking, = 0.811 226 © John Bird & Carl Ross Published by Taylor and Francis EXERCISE 91, Page 201 1. A conical pendulum rotates about a horizontal circle at 100 rpm. If the speed of rotation of the mass increases by 5%, how much does the mass of the pendulum rise ? Angular velocity, = 2n 2100 = 10.472 rad/s 60 60 g h = from which, height, h = or 2 = g h g 9.81 = = 0.089456 m 2 10.472 2 When the speed of rotation rises by 5%, n 2 = 100 1.05 = 105 rpm Hence, 2 = 2 = Hence, 2n 2 2105 = 10.996 rad/s 60 60 g h2 or 2 2 = h2 = g h2 9.81 g = 2 10.996 2 2 i.e. the new value of height, h 2 = 0.081133 m Rise in height of the pendulum mass = ‘old’ h – ‘new’ h = h - h 2 = 0.089456 – 0.081133 = 0.00832 m = 8.32 mm 2. If the speed of rotation of the mass of Problem 1 decreases by 5%, how much does the mass fall ? From Problem 1, h = 0.089456 m When the speed of rotation decreases by 5%, n 2 = 100 0.95 = 95 rpm Hence, 2 = 2n 2 2 95 = 9.9484 rad/s 60 60 227 © John Bird & Carl Ross Published by Taylor and Francis 2 = Hence, g h2 or 2 2 = h2 = g h2 9.81 g = 2 9.9484 2 2 i.e. the new value of height, h 2 = 0.099120 m Fall in height of the pendulum mass = ‘old’ h – ‘new’ h = h - h 2 = 0.089456 – 0.099120 = - 0.00966 m = 9.66 mm 3. A conical pendulum rotates at a horizontal angular velocity of 2 rad/s. If the length of the string is 3 m and the pendulum mass is 0.25 kg, determine the tension in the string. Determine also the radius of the turning circle. Angular velocity, = 2 rad/s Tension in the string, T = m 2 L = 0.25 kg (2 rad/s) 2 3 m T = 3 kg m/s 2 i.e. However, 1 kg m/s 2 = 1 N, hence, tension in the string, T = 3 N T= mg mg 0.25 kg 9.81m / s 2 from which, cos = = = 0.8175 cos T 3N Hence, the cone angle, = cos 1 (0.8175) = 35.165 sin = r , from which, radius of turning circle, r = L sin = 3 m sin 35.165 L = 1.728 m 228 © John Bird & Carl Ross Published by Taylor and Francis EXERCISE 92, Page 203 1. A uniform disc of diameter 0.1 m rotates about a vertical plane at 200 rpm. The disc has a mass of 1.5 kg attached at a point on its rim and another mass of 2.5 kg at another point on its rim, where the angle between the two masses is 90 clockwise. Determine the magnitude of the resultant centrifugal force that acts on the axis of the disc, and its position with respect to the 1.5 kg mass. Angular velocity, = 2n 2 200 = 20.944 rad/s 60 60 Force, F1 m12 r 1.5 20.9442 0.1 = 32.90 N 2 Force, F2 m 2 2 r 2.5 20.9442 0.1 = 54.83 N 2 From the diagram, resultant, R = F 2 1 F22 32.90 2 54.832 by Pythagoras = 63.94 N cos θ = and 32.90 32.90 = 0.515 R 63.94 θ = cos 1 (0.515) = 59º clockwise 2. If a mass of 4 kg is placed on some position on the disc in Problem 1, determine the position where this mass must be placed to nullify the unbalanced centrifugal force. From Problem 1, resultant, R = 63.94 N = m2 r i.e. from which, 63.94 = 4 20.9442 r radius, r = 63.94 = 0.03644 m 4 20.944 2 229 © John Bird & Carl Ross Published by Taylor and Francis Hence, radius, r = 36.44 mm at (180º - 59º) anticlockwise to the 1.5 kg mass i.e. radius r = 36.44 mm at 121º anticlockwise to the 1.5 kg mass 3. A stone of mass 0.1 kg is whirled in a vertical circle of 1 m radius by a mass-less string, so that the string just remains taut. Determine the velocity and tension in the string at (a) the top of the circle, (b) the bottom of the circle, (c) midway between (a) and (b). (a) At the top, tension T = 0 N m2 r mg i.e. angular velocity, and g 9.81 = 3.132 rad/s r 1 linear velocity, v = ωr = 3.132 rad/s × 1 m i.e. velocity at the top, v 1 = 3.132 m/s and the tension = 0 N (b) At the bottom, (kinetic energy + potential energy) top = (kinetic energy) bottom i.e. i.e. mv12 mv 2 2 mg 2 2 2 v 2 2 v12 4g = 3.132 2 4 9.81 = 49.049 230 © John Bird & Carl Ross Published by Taylor and Francis v2 49.049 = 7 m/s and v2 Tension at the bottom, T2 mg m r m g r 2 49 = 0.1 × 9.81 = 5.88 N 1 i.e. velocity at the bottom, v 2 = 7 m/s and the tension = 5.88 N (c) Mid-way, (kinetic energy + potential energy) top = (kinetic energy + potential energy) mid way mv32 mv12 mg 2 mg 1 2 2 i.e. v32 v12 2g i.e. = 3.132 2 2 9.81 = 29.4294 v2 29.4294 = 5.42 m/s and Tension mid-way, T3 mv32 0.1 5.422 = 2.94 N r 1 i.e. velocity mid-way, v 3 = 5.42 m/s and the tension = 2.94 N EXERCISE 93, Page 203 Answers found from within the text of the chapter, pages 196 to 203. EXERCISE 94, Page 203 1. (b) 2. (d) 3. (a) 4. (b) 5. (b) 231 © John Bird & Carl Ross Published by Taylor and Francis