8 Pages

HW 11

Course: PHYS 105, Spring 2011
School: NJIT
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(tp8327) pampalone HW#11 swaminathan (10500) This print-out should have 16 questions. Multiple-choice questions may continue on the next column or page find all choices before answering. 001 10.0 points A 3.41 kg ball is attached to a 13.3 N fish line. The ball is released from rest at the horizontal position (0 = 90 ). At what angle (measured from the vertical) will the fish line break? The acceleration of...

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(tp8327) pampalone HW#11 swaminathan (10500) This print-out should have 16 questions. Multiple-choice questions may continue on the next column or page find all choices before answering. 001 10.0 points A 3.41 kg ball is attached to a 13.3 N fish line. The ball is released from rest at the horizontal position (0 = 90 ). At what angle (measured from the vertical) will the fish line break? The acceleration of gravity is 9.8 m/s2 . Correct answer: 82.3765. Explanation: In the swing down to the breaking point, energy is conserved: m v2 2 m v2 . 2 g m cos = r m g r cos = At the breaking point, consider the radial forces: Fr = m ar T - m g cos = m v2 r T = 3 m g cos T = arccos 3mg = arccos 13.3 N 3(3.41 kg)(9.8 m/s2 ) 6. 7. 8. 9. mgL 10 kL - 10 g L m g- kL m L L correct 10 L 1 If the ball is allowed to fall, what is its speed when the system is swinging through the vertical and the spring is stretched an L amount L = , where L is the spring's 10 initial, unstretched length? 1. 2. 3. 4. kL - 11 g m kL - 22 g 10 m 10 g - k L2 mg kL m L 10 L 10 L 100 5. Not enough information is given. L + L = 82.3765 . 22 g - kL 10 m 002 (part 1 of 2) 10.0 points A ball of mass m is attached to a spring of negligible mass, and force constant k. The spring is freely pivoted at the opposite end from the ball, and the system is initially at rest and horizontal. Explanation: Using conservation of energy with E = K + Us + Ug and taking Ug = 0 at the instant the system is vertical we get Ei = Ef pampalone (tp8327) HW#11 swaminathan (10500) Ki + Usi + Ugi = Kf + Usf + Ugf 1 1 0 + 0 + m g (L + L) = m v 2 + k (L)2 2 2 1 1 L2 11 L = m v2 + k mg 10 2 2 100 2 22 m g L k L - = m v2 10 100 mL kL 22 g - = mv 2 10 10 m 22 g - kL 10 m L =v 10 2 wrong answer, since the mass m is neither moving in a circle nor at a constant speed. 004 (part 1 of 3) 10.0 points A projectile of mass 4.3 kg kg is shot horizontally with an initial speed of 17.5 m/s from a height of 22.7 m above a flat desert surface. The acceleration of gravity is 9.81 m/s2 . a) For the instant before the projectile hits the surface, find the work done on the projectile by gravity. Correct answer: 957.554 J. Explanation: Basic Concept: Wgravity = Ug = m g h Given: m = 4.3 kg h = 22.7 m g = 9.81 m/s2 Solution: Wgravity = (4.3 kg) (9.81 m/s2 ) (22.7 m) = 957.554 J . 003 (part 2 of 2) 10.0 points Having calculated the speed in the first part, now find the acceleration a of the ball at the point where it swings through the vertical position. kL 1. ^ j -g 10 m 2. ^ g - j 3. -^ j v2 11 L 10 correct kL -g 10 m kL - 2g 4. ^ j 110 m 5. 0 6. ^ 2g - j kL 110 m 7. ^ g j kL 10 m kL 9. ^ j +g 10 m Explanation: From Newton's 2nd Law, 8. ^ j ma = a =^ j Fi = ^ (k L) - ^ (m g) j j kL -g 10 m . 005 (part 2 of 3) 10.0 points b) Find the change in kinetic energy since the projectile was fired. Correct answer: 957.554 J. Explanation: Basic Concept: K = Wgravity Solution: K = 957.554 J . Note that substituting v 2 from part 1 into v2 v2 = will generate a completely a= r L + L 006 (part 3 of 3) 10.0 points c) Find the final kinetic energy of the projectile. pampalone (tp8327) HW#11 swaminathan (10500) Correct answer: 1615.99 J. Explanation: Basic Concept: K = Kf - Ki = Given: vi = 17.5 m/s Solution: Kf = K + Ki 1 = K + mvi 2 2 3. 4. 1 1 2 2 m vf - m vi 2 2 3 By how much has the spring stretched (or compressed) in the second situation described? 1. 2. 3m v0 correct 4k 5m v0 2k 7m v0 4k 1m v0 4k 5. None of these 7m v0 2k Explanation: In the first case, the total energy 6. E1 = K1 + K2 + Us 1 1 2 2 = m v0 + m v0 + 0 2 2 2 = m v0 . In the second case, the total energy E2 = K1 + K2 + Us 1 v0 2 1 1 2 = m + m v0 + k 2 2 2 2 2 1 5 2 = m v0 + k 2 . 8 2 Total energy is conserved, so E1 = E2 1 5 2 2 m v0 = m v0 + k 2 8 2 1 3 2 k 2 = m v0 2 8 3m v0 . = 4k The spring could be stretched ( > 0) or compressed ( < 0). 008 10.0 points A block of mass m is pushed a distance D up an inclined plane by a horizontal force F . The plane is inclined at an angle with respect to 1 = (957.554 J) + (4.3 kg) (17.5 m/s)2 2 = 1615.99 J . 007 10.0 points Two boxes of the same mass m are sliding without friction on a horizontal surface, connected by a spring of force constant k. At a certain instant the spring is unstretched and the two boxes are moving in the same direction at the same speed v0 . v0 v0 m L0 At another instant the leading box is moving at the same speed v0 as before, but the trailing box is moving in the same direction at only half its initial speed. v0 v0 2 m L0 + m m pampalone (tp8327) HW#11 swaminathan (10500) the horizontal. The block starts from rest and the coefficient of kinetic friction is k . D 4 F m k 009 10.0 points A 2.6 103 kg car accelerates from rest under the action of two forces. One is a forward force of 1151 N provided by traction between the wheels and the road. The other is a 937 N resistive force due to various frictional forces. How far must the car travel for its speed to reach 3.3 m/s? Correct answer: 66.1542 m. Explanation: Basic Concepts: 1 2 Wnet = K = Kf - Ki = mvf 2 1 2 since vi = 0 m/s Ki = mvi = 0 J. 2 Fnet = F1 - F2 Wnet = Fnet d cos = Fnet d since = 0 cos = 1. Given: m = 2.6 103 kg F1 = 1151 N F2 = 937 N vf = 3.3 m/s Solution: 1 2 (F1 - F2 ) d = mvf 2 2 mvf d= 2(F1 - F2 ) (2600 kg)(3.3 m/s)2 d= 2(1151 N - 937 N) = 66.1542 m What is the final speed of the block? 1. v = 2. v = correct 3. v = 4. v = 5. v = 6. v = 7. v = 8. v = 2 (F sin - k N ) D m 2 (F cos - m g sin - k N ) D m 2 (F cos + m g sin ) D m 2 (F cos + m g sin - k N ) D m 2 (F cos - m g sin ) D m 2 (F sin + k N ) D m 2 (F cos - m g sin + k N ) D m 2 cos (F - k N ) D m Explanation: The work done by gravity is Wgrav = m g D cos(90 + ) = -m g D sin . The work done by the force F is WF = F D cos . From the work-energy theorem we know that Wnet = K , WF + Wgrav + Wf riction = Thus vf = 2 (F cos - m g sin - k N ) D . m 1 2 m vf . 2 010 (part 1 of 3) 10.0 points A block is pushed against the spring with spring constant 14 kN/m (located on the lefthand side of the track) and compresses the pampalone (tp8327) HW#11 swaminathan (10500) spring a distance 5 cm from its equilibrium position (as shown in the figure below). The block starts at rest, is accelerated by the compressed spring, and slides across a frictionless track except for a small rough area on a horizontal section of the track (as shown in the figure below). It leaves the track horizontally, flies through the air, and subsequently strikes the ground. The acceleration of gravity is 9.8 m/s2 . 14 kN/m 5 cm 521 g 2.4 m 1.4 m =0.5 vx 5 1 1 2 m vx = k d2 - m g 2 2 k d2 2 vx = - 2g m Thus vx = k d2 -2g m (14000 N/m) (0.05 m)2 = 0.521 kg 1/2 - 2 (0.5) (9.8 m/s2 ) (1.4 m) = 7.31153 m/s . 011 (part 2 of 3) 10.0 points What is the horizontal distance x the block travels in the air? Correct answer: 5.11701 m. x What is the speed v of the block when it leaves the track? Correct answer: 7.31153 m/s. Explanation: Let : g = 9.8 m/s2 , m = 0.521 kg , k = 14000 N/m , v = vx , = 1.4 m , d = 0.05 m , and vf = 10.0249 m/s . vx d Explanation: Choosing the point where the block leaves the track as the origin of the coordinate system, x = vx t 1 y = - g t2 2 since axi = 0 m/s2 and vyi = 0 m/s. At y = h (below the jump off height), 1 h = - g t2 2 t= -2 h . g (8) (9) k h x Applying Conservation of Mechanical Energy, Ui = Uf + Kf + W since vi = 0 m/s. 1 1 Since K = m v 2 , Us = k d2 , and W = 2 2 mg, Since x = vx t , we have x = vx t = = k d2 - 2g m - -2 h g 2h k d2 -2g m g pampalone (tp8327) HW#11 swaminathan (10500) = - (14000 N/m) (0.05 m)2 (0.521 kg) Calculate the spring force constant k. Correct answer: 792.876 N/m. Explanation: 6 - 2 (0.5) (9.8 m/s2 ) (1.4 m) 2 (-2.4 m) (9.8 m/s2 ) = 5.11701 m . 1/2 Let : 012 (part 3 of 3) 10.0 points What is the total speed of the block when it hits the ground? Correct answer: 10.0249 m/s. Explanation: Kf = Ui , since vi = 0 m/s and hf = 0 m, so the vertical motion gives 1 2 m vy = m g h . 2 vy = = vf = = -2 g h -2 (9.8 m/s2 ) (-2.4 m) so 2 2 vx + vy m = 128 g , h = 65.7 cm , and x = 4.72041 cm . Using conservation of energy, we have 1 2 k x = m g (h + x) 2 from which k= 2 m g (h + x) x2 2 (0.128 kg)(9.8 m/s2 )(0.657 m + 0.0472041 m) = (0.0472041 m)2 = 792.876 N/m . = 6.85857 m/s , (7.31153 m/s)2 + (6.85857 m/s)2 = 10.0249 m/s . 013 10.0 points A(n) 128 g ball is dropped from a height of 65.7 cm above a spring of negligible mass. The ball compresses the spring to a maximum displacement of 4.72041 cm. The acceleration of gravity is 9.8 m/s2 . 014 10.0 points A spring with a spring-constant 3 N/cm is compressed 31 cm and released. The 8 kg mass skids down the frictional incline of height 37 cm and inclined at a 24 angle. The acceleration of gravity is 9.8 m/s2 . The path is frictionless except for a distance of 0.9 m along the incline which has a coefficient of friction of 0.5 . k = 3 N/cm 8 kg 37 cm 31 cm 24 = 0. 0. 9m vf h 5 Figure: Not drawn to scale. What is the final velocity vf of the mass? x Correct answer: 1.67281 m/s. Explanation: pampalone (tp8327) HW#11 swaminathan (10500) Multiplying by 2 and dividing by m gives us Let : g = 9.8 m/s2 = , k = 3 N/cm = 300 N/m , x = 31 cm = 0.31 m , = 0.5 , = 0.9 m , h = 0.37 m , m = 8 kg , and = 24 , 2 Kf = v 2 , so m 2 Kf v= m = 2 (11.1931 J) (8 kg) 7 = 1.67281 m/s . Consider the kinetic energy of the mass. The mass receives its initial kinetic energy from the potential energy of the spring Ki = Uspring 1 = k x2 2 1 = (300 N/m) (0.31 m)2 2 = 14.415 J . (1) It gains kinetic energy because of the potential energy lost in moving down the incline Kgained = Ulost = mgh (2) 2 = (8 kg) (9.8 m/s ) (0.37 m) = 29.008 J . and loses kinetic energy by doing work on the frictional surface Klost = Wf r = m g cos = (0.5) (8 kg) (9.8 m/s2 ) (0.9 m) cos(24 ) = 32.2299 J . (3) Alternate Explanation: The potential energy at the top of the hill will be converted into kinetic energy at the bottom of the hill minus energy lost due to the nonconservative friction force. The potential energy at the top of the hill consists of the gravitational potential energy plus the potential energy contained in the compressed spring. Combining Eqs. 1, 2, 3, and 4, we have v= 1 2 m g h + k x2 - m g cos m 2 015 (part 1 of 2) 10.0 points A 380 g particle in a semi-spherical bowl of radius 0.4 m is released from rest at point A at the level of the center of the bowl, and the surface of the bowl is rough. The speed of the particle at B is 2.3 m/s. The acceleration of gravity is 9.8 m/s2 . A R B Since energy is concerved, the final kinetic energy is Kf = Us + Ul - Wf r = (14.415 J) + (29.008 J) - (32.2299 J) = 11.1931 J . However, the final kinetic energy is Kf = 1 m v2 . 2 (3) What is its kinetic energy at B? Correct answer: 1.0051 J. Explanation: pampalone (tp8327) HW#11 swaminathan (10500) The kinetic energy at B is KB = 1 2 m vB 2 1 = (380 g)(0.001 kg/g)(2.3 m/s)2 2 = 1.0051 J . 8 016 (part 2 of 2) 10.0 points What is the magnitude of the energy lost due to friction as the particle moves from A to B? Correct answer: 0.4845 J. Explanation: The loss of energy is equal to the work done by the force of friction E = +U + K = -m g R + K = -(380 g) (9.8 m/s2 ) (0.4 m) + 1.0051 J = -0.4845 J |E| = 0.4845 J .
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Cornell - PAM - 4380
Outline: 2/21/2011 3.0 Prohibition Basic issues: supply &amp; demand (today) Examples Heroin and meth Readings: Weatherburn et al, Dobkin &amp; Nicosia Alcoholic beverages w/ caffeine Restaurant smoking bans Prelim #1: March 4 Homework #3 due Monday, 2/28/20
Cornell - PAM - 4380
Outline: 2/23/2011 Heroin and meth Drug policy analysis Heroin drought Background on Meth Next: War on meth (Dobkin &amp; Nicosia 2009) Alcoholic beverages w/ caffeine Homework #3: due Monday, Feb. 28 Prelim #1: Friday, March 3Drug Policy Analysis Inte
Cornell - PAM - 4380
2/25/2011 Supply-side intervention in the market for meth Dobkin &amp; Nicosia Alcoholic beverages with caffeine Next: restaurant smoking bans Shetty et al, 2009 Homework #3: due Monday, Feb. 28 Prelim #1: Friday, March 4War on Meth 1995 DEA raids Cli
Cornell - PAM - 4380
Obesity and Tax PolicyJohn Cawley PAM/ECON 4380 guest lecture April 6, 2011PAM-Econ 4280: Economics of Risky Health Behaviors I'll be teaching it Fall 2011 I ll With this course (4380), forms a two-course sequence in the economics and public policy of
Cornell - PAM - 4380
PAM 4380: 1/28/2011 Estimating actual causes of death: some of the details History of the field of epidemiology: Susser &amp; Susser 1996 Next time: economic approach to public health, Cawley 2004 Announcements: Course Blackboard site is up Reading packet r
Cornell - PAM - 4380
PAM 4380: 1/31/20112. Economics versus Public Health: An Overview 2.1 Normative Economics &amp; Public Health Ethics Brief introduction to positive health economics = framework used by economists as social scientists to understand health behaviors Constrain
Cornell - PAM - 4380
Health Information 03/16/2011 The truth campaign Background, research design, &amp; findings (Mon.) Discussion (today) Food advertising &amp; obesity (next) Homework #4 due FridayModel specification In addition to explanatory variables listed in Table: &quot;Cont
Cornell - PAM - 4380
Alcohol Taxation 4/1/2011 Alcohol taxation Pass-thru to prices Impact of prices on alcohol consumption &amp; alcohol-related problems Monday: &quot;Effect of Alcohol Tax Increase on Alcohol-Related Disease Mortality in Alaska&quot; (Wagenaar et al, AJPH August 2009)
Cornell - PAM - 4380
PAM 4380: 4/4/2011 Effect of Alcohol Tax Increase Wagenaar et al, AJPH, August 2009 Next time: Cawley on taxes &amp; obesity Homework #5 due Wednesday This presentation includes a revised and extended version of the graphs I drew on the board during lecture.
Cornell - PAM - 4380
April 8, 2011 6. LitigationBonus Topic: Behavioral Economics &amp; Taxation 6.1 Basic Issues and Analysis Jacobson and Warner (1999)6.2 Example: The Master Settlement Agreement Bulow and Klemperer (1998)6.4 Example: Obesity Lawsuits Alderman and Daynard
Cornell - PAM - 4380
Litigation 4/11/2011 Master Settlement Agreement Structure of cigarette industry (Bulow &amp; Klemperer) Impact of MSA on cigarette industry Impact of MSA funds Political theory Homework #6 due Monday, April 18 Obesity Lawsuits (probably next week) Prelim
Cornell - PAM - 4380
Litigation 4/13/2011 Master Settlement Agreement Impact on cigarette industry, cont. Next time: other impacts, political theory Next week: Obesity litigation Homework #6 due Monday Prelim #2: Friday, April 22 Covers information, taxation, litigationI
Cornell - PAM - 4380
Litigation 4/18/2011 Obesity lawsuits Homework #6: due today Prelim #2: Friday Covers information, taxation, litigationObesity Lawsuits Pelman v. McDonald's Corp. Class action suit: &quot;brought on behalf of children who consumed McDonald's products and a
Cornell - PAM - 4380
Litigation 4/20/2011Prelim #2 Friday, 4/22Covers information, taxation, litigationToday: impact of calorie posting in chain restaurantsClick to edit Master subtitle styleSupply &amp; demand graphs Review: Assume some tools.Impact of information Extern
Cornell - PAM - 4380
Health Information 3/14/2011 The truth campaign (today &amp; Wed.) Background Research design Findings Next time: discussion &amp; critique Homework #4 due Friday, March 19 Prelim Re-grade requests due Friday too1998 Settlement 1998 Master Settlement Agreeme