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Version 074 – Midterm 2 – OConnor (05141) This print-out should have 18 questions. Multiple-choice questions may continue on the next column or page – find all choices before answering. V1:1, V2:1, V3:3, V4:5, V5:5. BE SURE TO CIRCLE THE ANSWERS ON THE FRONT PAGES AND ATTACH YOUR WORK TO THE BACK. YOU MUST SHOW YOUR WORK! DO THE EASY PROBLEMS FIRST AND SAVE THE HARD ONES FOR LAST. 1 10. 5.08593 s Explanation: The initial x and y components of the velocity are vx0 = v0 cos θ0 = 12.3824 m/s vy0 = v0 sin θ0 = 9.81414 m/s . To find t, we can use the relation 1 2 gt 2 y = vy0 t − 001 (part 1 of 2) 10 points A stone is thrown from the top of a building upward at an angle of 38.4◦ to the horizontal and with an initial speed of 15.8 m/s, as in the figure. The height of the building is 53.2 m. The acceleration of gravity is 9.8 m/s2 . y v0 θ0 x with y = −53.2 m and vy0 = 9.81414 m/s (we have chosen the top of the building as the origin): 1 (9.81414 m/s) t − (9.8 m/s2 ) t2 2 = −53.2 m . 2 2 2 (4.9 m /s )t − (9.81414 m/s) t −53.2 m = 0 Applying the quadratic formula, since (−9.81414 m/s)2 − 4(4.9 m/s2 )(−53.2 m) = 1139.04 m2 /s2 , h then How long is the stone “in flight”? 1. 3.17932 s 2. 3.56725 s 3. 3.63387 s p 9.81414 m/s ± 1139.04 m2 /s2 t= 9.8 m/s2 = 4.44528 s 002 (part 2 of 2) 10 points What is the speed of the stone just before it strikes the ground? 1. 26.0056 m/s 4. 3.69763 s 2. 27.5092 m/s 5. 3.98715 s 3. 29.3169 m/s 6. 4.15309 s 4. 30.052 m/s 7. 4.3606 s 5. 33.1771 m/s 8. 4.44528 s correct 6. 34.7925 m/s 9. 4.78976 s 7. 35.9494 m/s correct Version 074 – Midterm 2 – OConnor (05141) 8. 36.8744 m/s 4. 40.1959 N 9. 38.0433 m/s 5. 41.1196 N 10. 40.1408 m/s Explanation: The y component of the velocity just before the stone strikes the ground can be obtained using the equation 8. 52.8437 N vy = vy0 − g t 9. 54.3434 N with t = 4.44528 s : 2 6. 42.8758 N 7. 49.7272 N 10. 56.8695 N Explanation: vy = (9.81414 m/s) − (9.8 m/s2 ) (4.44528 s) = −33.7496 m/s . Since vx = vx0 = 12.3824 m/s, the required speed is q v = vx2 + vy2 q = (12.3824 m/s)2 + (−33.7496 m/s)2 = 35.9494 m/s . 003 (part 1 of 3) 10 points A block of mass 1.91332 kg lies on a frictionless table, pulled by another mass 3.40141 kg under the influence of Earth’s gravity. The acceleration of gravity is 9.8 m/s2 . Given : m1 = 1.91332 kg , m2 = 3.40141 kg , µ = 0. a T T m1 N and m1 g m2 a m2 g The net force on the system is simply the weight of m2 . Fnet = m2 g = (3.40141 kg) (9.8 m/s2 ) = 33.3338 N . 1.91332 kg 004 (part 2 of 3) 10 points What is the magnitude of the acceleration a of the two masses? 1. 5.19695 m/s2 µ=0 3.40141 kg What is the magnitude of the net external force F acting on the two masses? 1. 29.6699 N 2. 5.63451 m/s2 3. 5.80805 m/s2 4. 6.27197 m/s2 correct 2. 31.0125 N 5. 6.36673 m/s2 3. 33.3338 N correct 6. 6.49314 m/s2 Version 074 – Midterm 2 – OConnor (05141) 7. 6.60275 m/s2 8. 6.82578 m/s2 9. 7.87789 m/s2 10. 8.06403 m/s2 Explanation: From Newton’s second law, 006 (part 1 of 3) 10 points A block is at rest on the incline shown in the figure. The coefficients of static and kinetic friction are µs = 0.7 and µk = 0.59, respectively. The acceleration of gravity is 9.8 m/s2 . 19 Fnet = m2 g = (m1 + m2 ) a . Solving for a, m2 g a= m1 + m 2 3.40141 kg = (9.8 m/s2 ) 1.91332 kg + 3.40141 kg = 6.27197 m/s2 . 005 (part 3 of 3) 10 points What is the magnitude of the tension T of the rope between the two masses? 1. 9.62636 N 3 kg µ What is the frictional force acting on the 19 kg mass? 1. 51.5525 N 2. 60.5674 N 3. 63.8114 N 4. 78.6916 N 2. 9.75315 N 5. 89.3359 N 3. 10.0116 N 6. 91.7786 N 4. 10.8381 N 7. 95.9001 N correct 5. 12.0003 N correct 8. 164.617 N 6. 14.1684 N 9. 181.3 N 7. 14.5665 N 10. 261.536 N Explanation: 8. 16.3735 N 9. 16.5868 N 10. 17.2402 N Explanation: Analyzing the horizontal forces on block m1 , we have X Fx : T = m 1 a = (1.91332 kg) (6.27197 m/s2 ) = 12.0003 N . 31◦ N Ff 31◦ mg Version 074 – Midterm 2 – OConnor (05141) The forces acting on the block are shown in the figure. Since the block is at rest, the magnitude of the friction force should be equal to the component of the weight on the plane of the incline Ff = M g sin θ = (19 kg) (9.8 m/s2 ) sin 31◦ = 95.9001 N . 007 (part 2 of 3) 10 points What is the largest angle which the incline can have so that the mass does not slide down the incline? 1. 19.7989 ◦ 2. 20.8068 ◦ 3. 22.7824 ◦ 4. 24.2277 ◦ 5. 27.0216 ◦ 6. 30.1137 ◦ 7. 33.0239 ◦ 8. 34.992 9. 36.1294 4 the incline if the angle of the incline is 39◦ ? 1. 0.854362 m/s2 2. 1.12114 m/s2 3. 1.24553 m/s2 4. 1.47742 m/s2 5. 1.49405 m/s2 6. 1.59314 m/s2 7. 1.61954 m/s2 8. 1.67388 m/s2 correct 9. 1.8754 m/s2 10. 2.06274 m/s2 Explanation: When θ exceeds the value found in part 2, the block starts moving and the friction force is the kinetic friction Fk = µk N = µk M g cos θ. Newton’s equation for the block then becomes ◦ correct ◦ 10. 36.8699 ◦ Explanation: The largest possible value the static friction force can have is Ff,max = µs N , where the normal force is N = M g cos θ. Thus, since Ff = M g sin θ, M g sin θm = µs M g cos θm tan θm = µs θm = tan−1 (µs ) = tan−1 (0.7) = 34.992◦ . 008 (part 3 of 3) 10 points What is the acceleration of the block down M a = M g sin θ − Ff = M g sin θ − µk M g cos θ and a = g [sin θ − µk cos θ] = (9.8 m/s2 ) [sin 39◦ − (0.59) cos 39◦ ] = 1.67388 m/s2 . 009 (part 1 of 1) 10 points As viewed by a bystander, a rider in a “barrel of fun” at a carnival finds herself stuck with her back to the wall. ω Version 074 – Midterm 2 – OConnor (05141) Which diagram correctly shows the forces acting on her? 5 The acceleration of gravity is 980 cm/s2 . What is the coefficient of static friction between the coin and the turntable? 1. 0.30012 2. 0.340136 correct 1. 3. 0.364431 4. 0.398288 2. 5. 0.445269 6. 0.507203 7. 0.522573 8. 0.565149 3. 9. 0.6387 4. correct 5. None of the other choices 6. Explanation: The normal force of the wall on the rider provides the centripetal acceleration necessary to keep her going around in a circle. The downward force of gravity is equal and opposite to the upward frictional force on her. Note: Since this problem states that it is viewed by a bystander, we assume that the free-body diagrams are in an inertial frame. 010 (part 1 of 1) 10 points A coin is placed 30 cm from the center of a horizontal turntable, initially at rest. The turntable then begins to rotate. When the speed of the coin is 100 cm/s (rotating at a constant rate), the coin just begins to slip. 10. 0.663265 Explanation: The normal force on the coin is N = m g . The force provided by friction immediately before slippage is given by f = µN = µmg. At this moment the centripetal acceleration (there is no tangential acceleration) provides a force m v2 F = . r Summation of forces yields m v2 , therefore r v2 µ= rg (100 cm/s)2 = (30 cm) (980 cm/s2 ) = 0.340136 . F = f = µmg = 011 (part 1 of 2) 10 points Consider the “loop-a-loop” setup, where a mass m is sliding along a frictionless track and the radius of the loop is R. Version 074 – Midterm 2 – OConnor (05141) C m R A D Given h = 5 R, determine the speed of the mass at A. p 1. |vA | = 2 2 g R correct p 2. |vA | = 2 g R p 3. |vA | = 4 g R p 4. |vA | = 3 g R p 5. |vA | = 3 2 g R p 6. |vA | = 4 2 g R Explanation: Applying the work energy theorem from C to A we get mgh − mgR = 1 2 m vA 2 mg(5 R − R) = 4 R m g = m v2 = mg. R Conservation of energy between C and B implies m g (h − 2 R) = 012 (part 2 of 2) 10 points Find the critical initial height of the mass, such that it would just barely pass the point B. 1 1 m v2 = m g R 2 2 m v2 R 5 R h = 2R + = R 2 2 mg = 013 (part 1 of 1) 10 points A(n) 88.3 g ball is dropped from a height of 66.1 cm above a spring of negligible mass. The ball compresses the spring to a maximum displacement of 4.6768 cm. The acceleration of gravity is 9.8 m/s2 . h 1 2 m vA 2 2 vA = 8gR p vA = 2 2 g R 1 1. h = R 2 2 2. h = R 3 5 3. h = R correct 2 3 R 2 1 5. h = R 3 Explanation: The critical condition at B implies that 4. h = B h 6 x Calculate the spring force constant k. 1. 324.238 N/m 2. 364.509 N/m 3. 511.447 N/m 4. 537.872 N/m 5. 560.028 N/m correct 6. 621.622 N/m 7. 702.946 N/m Version 074 – Midterm 2 – OConnor (05141) 8. 758.352 N/m 9. 851.065 N/m 7 9. 1.48144 m/s 10. 1.5 m/s Explanation: 10. 1028.17 N/m Explanation: Let : Let : m = 88.3 g , h = 66.1 cm , and x = 4.6768 cm . Using conservation of energy, we have m = 18.8 kg , M = 2170 kg , and v = 140 m/s . The cannon’s velocity immediately after it was fired is found by using conservation of momentum along the horizontal direction: 1 2 k x = m g (h + x) 2 M V + mv = 0 A revolutionary war cannon, with a mass of 2170 kg, fires a 18.8 kg ball horizontally. The cannonball has a speed of 140 m/s after it has left the barrel. The cannon carriage is on a flat platform and is free to roll horizontally. What is the speed of the cannon immediately after it was fired? 1. 0.797431 m/s = 1.2129 m/s . m v M from which where M is the mass of the cannon, V is the 2 m g (h + x) velocity of the cannon, m is the mass of the k= x2 cannon ball and v is the velocity of the cannon 2 (0.0883 kg)(9.8 m/s2 )(0.661 m + 0.046768 m) ball. Thus, the cannon’s speed is = (0.046768 m)2 m |v| |V | = = 560.028 N/m . M 18.8 kg = (140 m/s) 2170 kg 014 (part 1 of 2) 10 points 2. 0.872308 m/s 3. 1.12371 m/s ⇒ −V = 015 (part 2 of 2) 10 points The same explosive charge is used, so the total energy of the cannon plus cannonball system remains the same. Disregarding friction, how much faster would the ball travel if the cannon were mounted rigidly and all other parameters remained the same? 1. 0.397969 m/s 4. 1.14343 m/s 2. 0.435308 m/s 5. 1.16174 m/s 3. 0.560479 m/s 6. 1.2129 m/s correct 4. 0.570196 m/s 7. 1.37624 m/s 5. 0.579618 m/s 8. 1.42581 m/s 6. 0.605144 m/s correct Version 074 – Midterm 2 – OConnor (05141) 8 r m → v . M man ³m´ → =− v man . correct M 7. 0.686424 m/s 3. VEarth = − 8. 0.71115 m/s 4. VEarth 9. 0.738726 m/s 5. VEarth = + v man . µ ¶ M → v man . 6. VEarth = + m → 10. 0.747671 m/s Explanation: By knowing the speeds of the cannon and the cannon ball, we can find out the total kinetic energy available to the system Knet = 1 1 m v2 + M V 2 . 2 2 This is the same amount of energy available as when the cannon is fixed. Let v 0 be the speed of the cannon ball when the cannon is held fixed. Then, 1 1 m v 02 = (m v 2 + M V 2 ) . 2 2 r M 2 V v2 + m r m =v 1+ M s ⇒ v0 = = (140 m/s) 1+ 18.8 kg 2170 kg = 140.605 m/s . Thus, the velocity difference is v 0 − v = 140.605 m/s − 140 m/s → 7. VEarth = − v man . µ ¶ M → 8. VEarth = − v man . m Explanation: The momentum is conserved. We have → So → V Earth = − ³m´ M → v man . 017 (part 1 of 1) 10 points A child bounces a 55 g superball on the sidewalk. The velocity change of the superball is from 23 m/s downward to 17 m/s upward. If the contact time with the sidewalk is 1/800 s, what is the magnitude of the force exerted on the superball by the sidewalk? 1. 1414.4 N 2. 1452 N 3. 1480 N 4. 1545.6 N = 0.605144 m/s . 5. 1579.2 N 016 (part 1 of 1) 10 points Bill (mass m) plants both feet solidly on the ground and then jumps straight up with ve→ locity v . The earth (mass M ) then has velocity ³m´ → v man . 1. VEarth = + M r m → 2. VEarth = + v . M man → m v man + M V Earth = 0 6. 1640 N 7. 1680 N 8. 1760 N correct 9. 1788.8 N 10. 1856 N Explanation: Version 074 – Midterm 2 – OConnor (05141) Let : m = 55 g = 0.055 kg , vu = 17 m/s , vd = 23 m/s , and ∆t = 0.00125 s Choose the upward direction as positive. Then the impulse is I = F ∆t = ∆P = m vu − m (−vd ) = m (vu + vd ) m (vu + vd ) F = ∆t (55 g) (17 m/s + 23 m/s) = 0.00125 s = 1760 N . 018 (part 1 of 1) 10 points As shown in the top view above, a disc of mass m is moving horizontally to the right with speed v on a table with negligible friction when it collides with a second disc of mass 9 m. The second disc is moving horizontally v at the moment of to the right with speed 8 impact. The two discs stick together upon impact. v 8 v before m 9m vf after 10 m The speed of the composite body immediately after the collision is 1. vf = 2. vf = 3. vf = 4. vf = 5. vf = 6. vf = 7. vf = 8. vf = 9 11 v. 20 5 v. 9 17 v. correct 80 3 v. 10 1 v. 4 11 v. 35 7 v. 15 7 v. 27 9. None of these are correct. 1 v. 2 Explanation: The total momentum of the system is conserved because there is no exterior force. So what we have is v (m + 9 m) vf = m v + 9 m 8¶ µ 9 10 m vf = m v 1 + 8 µ ¶ 8 9 + 10 vf = v 8 8 17 v 10 vf = 8 (17) vf = v (8) (10) 17 = v , so 80 17 v . = 80 10. vf =