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UW-Madison PHYSICS 207 - Lecture 13

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Lecture 13Momentum is conserved if no external forceInelastic collision in 1-D: ExampleSlide 4Momentum is a vectorA perfectly inelastic collision in 2-DSlide 7Exercise Momentum is a Vector (!) quantityElastic CollisionsBilliardsBilliards: Without external forces, conservation of momentum (and energy Ch. 10 & 11)Explosions: A collision in reverseSlide 18Slide 19Impulse (A variable force applied for a given time)Force and Impulse (A variable force applied for a given time)Force and ImpulseAverage Force and ImpulseExercise Force & ImpulseBoxing: Use Momentum and Impulse to estimate g “force”Slide 26Ch. 10 : Kinetic & Potential energiesSlide 29Physics 207: Lecture 13, Pg 1Lecture 13Goals:Goals:Assignments: Assignments: HW5, due tomorrow HW5, due tomorrow For Wednesday, Read all of Chapter 10For Wednesday, Read all of Chapter 10•Chapter 9Chapter 9 Employ conservation of momentum in 1 D & 2D Examine forces over time (aka Impulse)•Chapter 10Chapter 10 Understand the relationship between motion and energyPhysics 207: Lecture 13, Pg 2Momentum is conserved if no external force afterbeforeppPhysics 207: Lecture 13, Pg 3Inelastic collision in 1-D: ExampleA block of mass M is initially at rest on a frictionless horizontal surface. A bullet of mass m is fired at the block with a muzzle velocity (speed) v. The bullet lodges in the block, and the block ends up with a final speed V. In terms of m, M, and V :What is the momentum of the bullet with speed v ?vVbefore afterxPhysics 207: Lecture 13, Pg 4Inelastic collision in 1-D: ExampleWhat is the momentum of the bullet with speed v ? Key question: Is there a net external x-dir force ? If not, then momentum in the x-direction is conserved!vVbefore afterxaaaavm 0 M v m V)/1( v mMP BeforeP After V)( Mm Physics 207: Lecture 13, Pg 5Momentum is a vectorzzyxxmpmpmpkjimpvvvˆpˆpˆpvyzyxPhysics 207: Lecture 13, Pg 6A perfectly inelastic collision in 2-DConsider a collision in 2-D (cars crashing at a slippery intersection...no friction).v1v2 beforem1m2If no external force momentum is conserved.Momentum is a vector so px, py and pz V afterm1 + m2Physics 207: Lecture 13, Pg 7A perfectly inelastic collision in 2-Dv1v2 V before afterm1m2m1 + m2x-dir px : m1 v1 = (m1 + m2 ) V cos y-dir py : m2 v2 = (m1 + m2 ) V sin p1p2pPhysics 207: Lecture 13, Pg 8Exercise Momentum is a Vector (!) quantityA. YesB. NoC. Yes & NoD. Too little information givenA block slides down a frictionless ramp and then falls and lands in a cart which then rolls horizontally without frictionIn regards to the block landing in the cart is momentum conserved?Physics 207: Lecture 13, Pg 12Elastic CollisionsElastic means that the objects do not stick.There are many more possible outcomes but, if no external force, then momentum will always be conservedStart with a 1-D problem.Before AfterPhysics 207: Lecture 13, Pg 13BilliardsConsider the case where one ball is initially at rest. pa  pb FPa beforeafterThe final direction of the red ball will depend on where the balls hit.Physics 207: Lecture 13, Pg 14Billiards: Without external forces, conservation of momentum (and energy Ch. 10 & 11)Conservation of Momentumx-dir Px : m vbefore = m vafter cos + m Vafter cos  y-dir Py : 0 = m vafter sin + m Vafter sin  pafter  ppb FPafter beforeafterPhysics 207: Lecture 13, Pg 17Explosions: A collision in reverseA two piece assembly is hanging vertically at rest at the end of a 2.0 m long massless string. The mass of the two pieces are 60 and 20 kg respectively. Suddenly you observe that the 20 kg is ejected horizontally at 30 m/s. The time of the “explosion” is short compared to the swing of the string.Does the tension in the string increase or decrease after the explosion?BeforeAfterPhysics 207: Lecture 13, Pg 18Explosions: A collision in reverseA two piece assembly is hanging vertically at rest at the end of a 2.0 m long massless string. The mass of the two pieces are 60 and 20 kg respectively. Suddenly you observe that the 10 kg is ejected horizontally at 30 m/s. Decipher the physics:1. The green ball recoils in the –x direction (3rd Law) and, because there is no net force in the x-direction the x-momentum is conserved. 2. The motion of the green ball is constrained to a circular path…there must be centripetal (i.e., radial acceleration)BeforeAfterPhysics 207: Lecture 13, Pg 19Explosions: A collision in reverseA two piece assembly is hanging vertically at rest at the end of a 20.0 m long massless string. The mass of the two pieces are 60 & 20 kg respectively. Suddenly you observe that the 20 kg mass is suddenly ejected horizontally at 30 m/s. Cons. of x-momentumPx before= Px after = 0 = - M V + m v V = m v / M = 20*30/ 60 = 10 m/sTbefore = Weight = (60+20) x 10 N = 800 NFy = m ay (radial) = M V2/r = T – MgT = Mg + MV2 /r = 600 N + 60x(10)2/20 N = 900 NBeforeAfterPhysics 207: Lecture 13, Pg 20Impulse (A variable force applied for a given time) Gravity: At small displacements a “constant” forceSprings often provide a linear force (-kx) towards its equilibrium position (Chapter 10)Collisions often involve a varying force F(t): 0  maximum  0We can plot force vs time for a typical collision. The impulse, J, of the force is a vector defined as the integral of the force during the time of the collision.Physics 207: Lecture 13, Pg 21Force and Impulse (A variable force applied for a given time) Fpttpdd td tpdd tFJ)/(J a vector that reflects momentum transfertti tft Impulse J = area under this curve !(Transfer of momentum !)Impulse has units of Newton-secondsPhysics 207: Lecture 13, Pg 22Force and ImpulseTwo different collisions can have the same impulse since JJ depends only on the momentum transfer, NOT the nature of the collision.t FtFtt same areat big, FF smallt small, FF bigPhysics 207: Lecture 13, Pg 23Average Force and ImpulseAverage Force and Impulset FtFtt t big, Fav smallt small, Fav bigFFav av FFav avPhysics 207: Lecture 13, Pg 24Exercise Force & ImpulseA. heavierB. lighterC. sameD. can’t tellTwo boxes, one heavier than the other, are initially at rest on a horizontal frictionless surface. The same constant force F acts on each one for exactly 1 second. Which box has the


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UW-Madison PHYSICS 207 - Lecture 13

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