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Brown - ECON - 206
EC 206 Microeconomics II: Second Midterm Exam April 9, 2007 (Professor Glenn C. Loury) ANSWERS 1. {35 points} Three bidders participate in the auction sale of a single object which is worth vi to bidder i , where vi is uniformly distributed on the un
Brown - ECON - 206
Microeconomic Theory II Assignment 3: Applications of Stochastic Dominance SolutionsFebruary 21, 2007Problem 1. Let 0 be a random variable representing a workers true ability. worker ability, i = 1, 2, with test scores t1 and t2 given by: t1 = +
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Solution of Racing Problem in Assignment 7 [Racing Game] Let V be the value of the prize, and let C(x) be the cost to a player of taking a step toward the nish line of size x. A player gets to move every sec
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Solution of Racing Problem in Assignment 7 [Racing Game] Let V be the value of the prize, and let C(x) be the cost to a player of taking a step toward the nish line of size x. A player gets to move every sec
Brown - ECON - 206
Microeconomic Theory II Assignment 4: Using Game Theory SolutionsFebruary 25, 2007Problem 1. Consider the simple duopoly model with linear demand: Two rms produce a homogeneous good for sale in a market with the inverse demand curve P = Max{d Q, 0
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Assignment 8: Signalling Games (1) Consider the following Grade Ination Problem: A professor must issue an evaluation of his student to the market. The professor perfectly observes his students productivity,
Brown - ECON - 206
Microeconomic Theory II Assignment 5: Game Theory SolutionsMarch 10, 2007Problem 1. [MWG 8.D.3] Consider a rst-price sealed-bid auction of an object with two bidders. Each bidder is valuation of the object is vi , which is known to both bidders. Ea
Brown - ECON - 206
EC 206 Microeconomics II: Final Examination May 4, 2007 (Professor Glenn C. Loury) Answers 1. {50 points} (A Principal-Agent Problem) The value of the project is the maximal net surplus that can be realized by exerting costly eort which raises the ch
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Assignment 2: Risk and Information 1. Concerning Measures of Risk Aversion: Let ui : , i = 1, 2, be two strictly increasing, strictly concave, twice dierentiable Bernoulli utility functions; and, let F : [
Brown - ECON - 206
EC 206 Microeconomics II: Second Midterm Exam April 9, 2007 (Professor Glenn C. Loury) Instructions. Please answser each of the three questions below. You do NOT need to use separate blue books for each question, but be sure to put your name and ID #
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Assignment 3: Applications of Stochastic Dominance 1. Let 0 be a random variable representing a workers true ability. tests of worker ability, i = 1, 2, with test scores t1 and t2 given by: t1 = + and t2
Brown - ECON - 206
EC 206 Microeconomics II First Midterm Exam February 28, 2007 Professor Glenn C. Loury Instructions. Please answser each of the three questions below. Use a separate blue book for each question. Be sure to put your name, ID #, and the question # on e
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Assignment 1: Choice under Uncertainty 1. Concerning the Independence Axiom: L L [0, 1], L : L + (1 )L L + (1 )L(a) (The Axiom extends to strict preference and to indierence.) Show that the Independen
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) A Note on Stochastic Dominance (February 8, 2007) Here are a few observations on stochastic dominance that may help with the material in yesterdays lecture. We will study the partial orderings of probability
Brown - ECON - 206
Microeconomic Theory II Assignment 7: Even more on Game Theory and some Externalities and Public Goods SolutionsApril 4, 2007Problem 1. Consider the following extensive form game of complete information (analogous to the partnership game studied by
Brown - ECON - 206
Economics 206 Spring 2007 (Prof. G. Loury) Assignment 8: The Principal-Agent Problem (1) A principal needs to contract with an agent to get a risky project done. The project can either succeed or fail. If it succeeds it generates output with gross va
Brown - ECON - 206
Microeconomic Theory II Assignment 5: Game Theory SolutionsMarch 10, 2007Problem 1. [MWG 8.D.3] Consider a rst-price sealed-bid auction of an object with two bidders. Each bidder is valuation of the object is vi , which is known to both bidders. Ea
Brown - ECON - 1210
CHAPTER13Aggregate SupplyQuestions for Review1. In this chapter we looked at three models of the short-run aggregate supply curve. All three models attempt to explain why, in the short run, output might deviate from its long-run "natural rate"
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 1.x = t 2 - ( t - 3) m3v=a= (a) Time at a = 0.dx 2 = 2t - 3 ( t - 3) m/s dtdv = 2 - 6 ( t - 3) m/s 2 dt0 = 2 - 3 ( t0 - 3) = 10 - 3t0t0 =10 3t0 = 3.33
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 9.a = 3e- 0.2t 0 dv = 0 a dtv -0=t 3e- 0.2t dt 0vt3 = e- 0.2t - 0.2t0v = -15 e- 0.2t - 1 = 15 1 - e- 0.2t At t = 0.5 s,()()v = 1.427 ft/sv
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 10.Given:a = - 5.4sin kt ft/s 2 ,t tv0 = 1.8 ft/s, x0 = 0, 5.4 cos kt ktk = 3 rad/sv - v0 = 0 a dt = - 5.4 0 sin kt dt = v - 1.8 = Velocity:05.4 ( cos
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 11.Given:a = - 3.24sin kt - 4.32 cos kt ft/s 2 ,x0 = 0.48 ft,tk = 3 rad/sv0 = 1.08 ft/st tv - v0 = 0 a dt = - 3.24 0 sin kt dt - 4.32 0 cos kt dt v - 1.
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 12.Given: At t = 0,v = 400 mm/s; a = kt mm/s 2 at t = 1 s, where k is a constant. x = 500 mmv = 370 mm/s, 1v t t 2 400 dv = 0 a dt = 0 kt dt = 2 ktv - 400 =
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 13.Determine velocity.v t t - 0.15 dv = 2 a dt = 2 0.15 dtv - ( -0.15 ) = 0.15t - ( 0.15 )( 2 ) v = 0.15t - 0.45 m/sAt t = 5 s,When v = 0, For 0 t 3.00 s,
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 59. Define positions as positive downward from a fixed level. Constraint of cable.( xB - xA ) + ( xC- x A ) + 2 ( xC - xB ) = constant3xC - xB - 2 x A = constant
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 59. Define positions as positive downward from a fixed level. Constraint of cable.( xB - xA ) + ( xC- x A ) + 2 ( xC - xB ) = constant3xC - xB - 2 x A = constant
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 44.Choose x positive upward. Rocket launch data: Constant acceleration a = - gRocket A:x = 0, v = v0 , t = 0 x = 0, v = v0 , t = t B = 4 sRocket B: Velocities:
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 29.x as a function of v. v = 1 - e-0.00057 x 154 v e -0.00057 x = 1 - 154 v 2 - 0.00057 x = ln 1 - 154 v 2 x = -1754.4 ln 1 - 154 a as a
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 14.Given: Separate variables and integrate.v t 2 0 dv = a dt = 0 ( 9 - 3t ) dt = 9a = 9 - 3t 2v - 0 = 9 t - t3 (a) When v is zero. t (9 - t 2 ) = 0 t = 0 and
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 45.(a) Acceleration of A.v A = ( v A )0 + a At ,( v A )0 = 168 km/h = 46.67 m/sv A = 228 km/h = 63.33 m/sAt t = 8 s,aA = v A - ( v A )0 t=63.33 - 46.67 8 1
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 30.Given: v = 7.5 (1 - 0.04 x )0.3with units km and km/h(a) Distance at t = 1 hr. Using dx = v dt , we get dt = dx dx = v 7.5(1 - 0.04 x)0.3Integrating, using
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 15.Given: Separate variables Integrate using dv = kt2 dt v = 10 m/s when t = 0 and v = 10 m/s when t = 2 s. a= dv = kt 2 dt10 2 2 -10 dv = 0 kt dtv10 - 10=
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 20.Note that a is a given function of x.7 a = 12 x - 28 = 12 x - m/s 2 3 7 Use v dv = a dx = 12 x - dx with the limits v = 8 m/s when x = 0. 3 v v dv 8
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 24.Given: a =v dv = - kv2 dxSeparate variables and integrate using v = 9 m/s when x = 0.v x 9 v = - k 0 dxdvln Calculate k using v = 7 m/s when x = 13 m. ln
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 3.Position:Velocity: x = 5t 4 - 4t 3 + 3t - 2 ft v= a= dx = 20t 3 - 12t 2 + 3 ft/s dt dv = 60t 2 - 24t ft/s 2 dtAcceleration:When t = 2 s,x = ( 5 )( 2 ) - ( 4 )
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 46.(a) Acceleration of A.v A = ( v A )0 + a At andand andx A = ( x A )0 + ( v A )0 t =1 a At 2 2Using( v A )0 = 0v A = a At( xA )0 = 0 givesxA = 1 a At
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 31.The acceleration is given by v dv gR 2 =a=- 2 dr r gR 2dr r2Then,v dv = -Integrating, using the conditions v = 0 at r = , and v = vesc at r = R0 2 vesc v
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 16.Note that a is a given function of x. a = 40 - 160 x = 160 ( 0.25 - x )(a) Note that v is maximum when a = 0, or x = 0.25 m Use v dv = a dx = 160 ( 0.25 - x ) dx
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 24.Given: a =v dv = - kv2 dxSeparate variables and integrate using v = 9 m/s when x = 0.v x 9 v = - k 0 dxdvln Calculate k using v = 7 m/s when x = 13 m. ln
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 60.Define positions as positive downward from a fixed level. Constraint of cable:( xB xA ) + ( xC x A ) + 2 ( xC xB ) = constant 3xC xB 2 x A = constant 3vC
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 61.Let x be position relative to the support taken positive if downward. Constraint of cable connecting blocks A, B, and C:2x A + 2 xB + xC = constant,2v A + 2vB
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 187.Let x be position relative to the fixed supports, taken positive if downward. Constraint of cable on left: 2v A + 3vB = 0, Constraint of cable on right: vB + 2vC
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 141.For uniformly decelerated motion: At t = 9 s,v = v0 + at t0 = 150 at ( 9 ) ,orat = 16.667 ft/s 22 a 2 = at2 + anTotal acceleration: an = a 2 at2
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 137.an =v2,at = 0,2 vmax = an2 vmax = ( 25)( 3g ) = ( 25 )( 3)( 9.81) = 735.35 m 2 /s 2vmax = 27.125 m/svmax = 97.6 km/h !Vector Mechanics for Eng
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 140.Length of run. Radius of circle.L = D = 130 meters(1)=1 D = 65m 2Tangential acceleration of starting portion of run. vm = at t1 = ( at )( 4 ) = 4 at
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 155.For the sun, andg = 274 m/s 2 ,R= 1 1 D = 1.39 109 = 0.695 109 m 2 2()Given that an =gR 2 v2 and that for a circular orbit an = r r2 r= gR 2 v2El
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 156.For the sun, andg = 274 m/s 2 R= 1 1 D = 1.39 109 = 0.695 109 m 2 2()Given that an =gR 2 v2 and that for a circular orbit: an = r r2 r= gR 2 v2El
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 99.(a) At the landing point, Horizontal motion: Vertical motion: from whichy = x tan 30 x = x0 + ( vx )0 t = v0t y = y0 + v y t2 = ( )0 t 1 gt 2 = 1 gt 2 2 2
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 149.Given: Differentiating twicex=( t 4 )36+ t2 my=t 3 ( t 1) m 6 42vx( 2 )2 & =x=2+ ( 2 )( 2 ) = 6 m/s t 2 ( t 1) m/s 2 2 1 & = t m/s 2 y
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 168.Change to rectangular coordinates.cos =r=x randsin =y rEquation of the path:3 3 3r = = yx sin cos yx rr or y = x + 3.from whichAlso,yx=3
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 143.(a)v A = 420 km/h v B = v A + v B/ Aor,v B = 520 km/h60v B/ A = v B v A = v B + ( v A )Sketch the vector addition as shown.2 2 2 vB/ A = v A + vB
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 167.Differentiate the expressions for r and with respect to time.r = 6t 1 + 4t 2 ,& r = 6 1 + 4t 2 + 24t 2 1 + 4t 2 & = 72t 1 + 4t 2 r()1 2()1 2 9
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 151.Let be the slope angle of the trajectory at an arbitrary point C. Then,( aC )n = gcos=C2 vC,orC =2 vC gcosBut, the horizontal component of vel
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 160.Radius of Earth Radius of orbit Normal accelerationR = ( 3960 mi )( 5280 ft/mi ) = 20.908 106 ft r = ( 3960 + 10900 )( 5280 ) = 78.4608 106 ft an = gR 2 r2 a
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 170.From geometry, Differentiating with respect to time, Transverse component of acceleration& & a = r + 2r =r=b cos& r= & b sin 2 cos & & b 2b sin 2 + 2 c
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 182.From problem 11.97, the position vector isr = ( Rt cos nt ) i + ctj + ( Rt sin nt ) k.Differentiating to obtain v and a, dr v= = R ( cos nt nt sin nt )
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 183.For A = 3 and B = 1, r = ( 3t cos t ) i + 3 t 2 + 1 j + ( t sin t ) k Differentiating to obtain v and a.v= a= dr t = 3 ( cos t t sin t ) i + 3 j + ( sin t + t
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 188.(a)Construction of the curves. Construct the at curve.0 < t < 10 s:10 s < t < 26 s: 26 s < t < 41 s: 41 s < t < 46 s: 46 s < t < 50 s:a = slope of v t cur
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 191.The horizontal and vertical components of velocity arevx = v0 sin15 v y = v0 cos15 gt At point B,vx v0 sin15 = = tan12 v y v0 cos15 gtorv0 sin15 + v0 co
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 192.First determine the velocity vC of the coal at the point where the coal impacts on the belt. Horizontal motion:( vC ) x = ( vC ) x 0 = 1.8cos 50 = 1.1570 m/s
LSU - CE - 2460
COSMOS: Complete Online Solutions Manual Organization SystemChapter 11, Solution 193.Given: Then, (a)t = 0,( vA )0 = 0,( a A )t =dv A = 0.8 in./s 2 dtv A = ( v A )0 + ( a A )t t = 0.8 tv A = 0,( a A )n =2 vA=0a A = ( a A )t (b