8.01SC Chapter 15: Collision Theory

Chapter 15 Collision Theory 15.1 Introduction........................................................................................................... 1 15.2 Reference Frames and Relative Velocities.......................................................... 1 15.2.1 Relative Velocities .......................................................................................... 3 15.2.2 Center-of-mass Reference Frame ................................................................. 4 15.2.3 Kinetic Energy in the Center-of-Mass Reference Frame ........................... 5 15.2.4 Change of Kinetic Energy and Relatively Inertial Reference Frames...... 5 15.3 Characterizing Collisions ..................................................................................... 7 15.4 One-Dimensional Collisions Between Two Objects........................................... 7 15.4.1 One Dimensional Elastic Collision in Laboratory Reference Frame ........ 7 15.4.2 One-Dimensional Collision Between Two Objects – Center-of-Mass Reference Frame ..................................................................................................... 11 15.5 Worked Examples............................................................................................... 12 Example 15.1 Elastic One-Dimensional Collision Between Two Objects .......... 12 Example 15.2 The Dissipation of Kinetic Energy in a Completely Inelastic Collision Between Two Objects ............................................................................. 13 Example 15.3 Bouncing Superballs ....................................................................... 14 15.6 Two Dimensional Elastic Collisions .................................................................. 17 15.6.1 Two-dimensional Elastic Collision in Laboratory Reference Frame...... 17 Example 15.5 Elastic Two-dimensional collision of identical particles.............. 20 Example 15.6 Two-dimensional elastic collision between particles of equal mass ................................................................................................................................... 21 Example 15.7 Two dimensional collision between particles of unequal mass ... 22 15.7 Two-Dimensional Collisions in Center-of-Mass Reference Frame ................ 24 15.7.1 Two-Dimensional Collision in Center-of-Mass Reference Frame........... 24 15.7.2 Scattering in the Center-of-Mass Reference Frame ................................. 25 Example 15.8 Scattering in the Lab and CM Frames ......................................... 26 Chapter 15 Collision Theory Despite my resistance to hyperbole, the LHC [Large Hadron Collider] belongs to a world that can only be described with superlatives. It is not merely large: the LHC is the biggest machine ever built. It is not merely cold: the 1.9 kelvin (1.9 degrees Celsius above absolute zero) temperature necessary for the LHC’s supercomputing magnets to operate is the coldest extended region that we know of in the universe—even colder than outer space. The magnetic field is not merely big: the superconducting dipole magnets generating a magnetic field more than 100,000 times stronger than the Earth’s are the strongest magnets in industrial production ever made. And the extremes don’t end there. The vacuum inside the proton-containing tubes, a 10 trillionth of an atmosphere, is the most complete vacuum over the largest region ever produced. The energy of the collisions are the highest ever generated on Earth, allowing us to study the interactions that occurred in the early universe the furthest back in time.1 Lisa Randall 15.1 Introduction When discussing conservation of momentum, we considered examples in which two objects collide and stick together, and either there are no external forces acting in some direction (or the collision was nearly instantaneous) so the component of the momentum of the system along that direction is constant. We shall now study collisions between objects in more detail. In particular we shall consider cases in which the objects do not stick together. The momentum along a certain direction may still be constant but the mechanical energy of the system may change. We will begin our analysis by considering two-particle collision. We introduce the concept of the relative velocity between two particles and show that it is independent of the choice of reference frame. We then show that the change in kinetic energy only depends on the change of the square of the relative velocity and therefore is also independent of the choice of reference frame. We will then study one- and two-dimensional collisions with zero change in potential energy. In particular we will characterize the types of collisions by the change in kinetic energy and analyze the possible outcomes of the collisions. 15.2 Reference Frames and Relative Velocities  We shall recall our definition of relative inertial reference frames. Let R be the vector from the origin of frame S to the origin of reference frame S′ . Denote the 1 Randall, Lisa, Knocking on Heaven's Door: How Physics and Scientific Thinking Illuminate the Universe and the Modern World, Ecco, 2011. 15-1  position vector of the j th particle with respect to the origin of reference frame S by r j and similarly, denote the position vector of the j th particle with respect to the origin of  reference frame S′ by r ′j (Figure 15.1). j th particle rj rj R S S Figure 15.1 Position vector of j th particle in two reference frames. The position vectors are related by    r j = r′j + R . (15.2.1) The relative velocity (call this the boost velocity) between the two reference frames is given by   dR . (15.2.2) V= dt Assume the boost velocity between the two reference frames is constant. Then, the relative acceleration between the two reference frames is zero,    dV A= =0. dt (15.2.3) When Eq. (15.2.3) is satisfied, the reference frames S and S′ are called relatively inertial reference frames. Suppose the j th particle in Figure 15.1 is moving; then observers in different reference frames will measure different velocities. Denote the velocity of j th particle in   frame S by v j = dr j / dt , and the velocity of the same particle in frame S′ by   v′j = dr ′j / dt . Taking derivative, the velocities of the particles in two different reference frames are related according to    v j = v′j + V . (15.2.4) 15-2 15.2.1 Relative Velocities Consider two particles of masses m1 and m2 interacting via some force (Figure 15.2). Figure 15.2 Two interacting particles Choose a coordinate system (Figure 15.3) in which the position vector of body 1 is given   by r1 and the position vector of body 2 is given by r2 . The relative position of body 1    with respect to body 2 is given by r1,2 = r1 − r2 . Figure 15.3 Coordinate system for two bodies.  During the course of the interaction, body 1 is displaced by dr1 and body 2 is displaced  by dr2 , so the relative displacement of the two bodies during the interaction is given by    dr1,2 = dr1 − dr2 . The relative velocity between the particles is    dr1,2 dr1 dr2    = − = v1 − v 2 . v1,2 = dt dt dt (15.2.5) We shall now show that the relative velocity between the two particles is independent of the choice of reference frame providing that the reference frames are relatively inertial.  ′ in reference frame S′ can be determined from using Eq. The relative velocity v12 (15.2.4) to express Eq. (15.2.5) in terms of the velocities in the reference frame S′ ,           v1, 2 = v1 − v 2 = (v1′ + V) − (v ′2 + V) = v1′ − v′2 = v1,′ 2 (15.2.6) 15-3 and is equal to the relative velocity in frame S . For a two-particle interaction, the relative velocity between the two vectors is independent of the choice of relatively inertial reference frames. 15.2.2 Center-of-mass Reference Frame  Let rcm be the vector from the origin of frame S to the center-of-mass of the system of particles, a point that we will choose as the origin of reference frame Scm , called the center-of-mass reference frame. Denote the position vector of the j th particle  with respect to origin of reference frame S by r j and similarly, denote the position  vector of the j th particle with respect to origin of reference frame Scm by r′j (Figure 15.4). j th particle rj rj rcm Scm S Figure 15.4 Position vector of j th particle in the center-of-mass reference frame. The position vector of the j th particle in the center-of-mass frame is then given by    r′j = r j − rcm . (15.2.7) The velocity of the j th particle in the center-of-mass reference frame is then given by    v′j = v j − v cm . (15.2.8) There are many collision problems in which the center-of-mass reference frame is the most convenient reference frame to analyze the collision. Consider a system consisting of two particles, which we shall refer to as particle 1 and particle 2. We can use Eq. (15.2.8) to determine the velocities of particles 1 and 2 in the center-of-mass,   m2 µ        m1v1 + m2 v 2 v1′ = v1 − v cm = v1 − = ( v1, − v 2 ) = v1, 2 . m1 + m2 m1 m1 + m2 (15.2.9) 15-4    where v12 = v1 − v 2 is the relative velocity of particle 1 with respect to particle 2 . A similar result holds for particle 2 :   m1 µ      m1v1 + m2 v 2   v′2 = v 2 − v cm = v 2 − =− ( v1 − v 2 ) = − v1, 2 . m1 + m2 m2 m1 + m2 (15.2.10) The momentum of the system the center-of-mass reference frame is zero as we expect,      m1v1′ + m2 v′2 = µ v12 − µ v12 = 0 . (15.2.11) 15.2.3 Kinetic Energy in the Center-of-Mass Reference Frame The kinetic energy in the center of mass reference frame is given by K cm = 1   1   m v ′ ⋅ v ′ + m v′ ⋅ v ′ . 2 1 1 1 2 2 2 2 (15.2.12) We now use Eqs. (15.2.9) and (15.2.10) to rewrite the kinetic energy in terms of the    relative velocity v12 ′ = v1′ − v ′2 , K cm = 1 ⎛ µ  ⎞ ⎛ µ  ⎞ 1 ⎛ µ  ⎞ ⎛ µ  ⎞ v v ⋅ − v m ⋅ + m − v 2 1 ⎜⎝ m1 1, 2 ⎟⎠ ⎜⎝ m1 1, 2 ⎟⎠ 2 2 ⎜⎝ m2 1, 2 ⎟⎠ ⎜⎝ m2 1, 2 ⎟⎠ 1⎞ 1 1   ⎛ 1 = µ 2 v1, 2 ⋅ v1, 2 ⎜ + ⎟ = µv1, 2 2 2 ⎝ m1 m2 ⎠ 2 . (15.2.13) where we used the fact that we defined the reduced mass by 1 1 1 . ≡ + µ m1 m2 (15.2.14) 15.2.4 Change of Kinetic Energy and Relatively Inertial Reference Frames The kinetic energy of the two particles in reference frame S is given by KS = 1 1 m1v12 + m2 v2 2 . 2 2 (15.2.15) We can take the scalar product of Eq. (15.2.8) to rewrite Eq. (15.2.15) as 15-5 1 1         m1 (v1′ + v cm ) ⋅(v1′ + v cm ) + m2 (v′2 + v cm ) ⋅(v′2 + v cm ) 2 2 . 1    2 1 2 1 2 = m1v1′ + m2 v2′ + (m1 + m2 )vcm + (m1v1′ + m2 v′2 ) ⋅ v cm 2 2 2 KS = (15.2.16) The last term is zero due to the fact that the momentum of the system in the center of mass reference frame is zero (Eq. (15.2.11)). Therefore Eq. (15.2.16) becomes KS = 1 1 1 m1v1′ 2 + m2 v2′ 2 + (m1 + m2 )vcm 2 . 2 2 2 (15.2.17) The first two terms correspond to the kinetic energy in the center of mass frame, thus the kinetic energies in the two reference frames are related by 1 K S = K cm + (m1 + m2 )vcm 2 . 2 (15.2.18) We now use Eq. (15.2.13) to rewrite Eq. (15.2.18) as KS = 1 1 µv1, 2 2 + (m1 + m2 )vcm 2 2 2 (15.2.19) Even though kinetic energy is a reference frame dependent quantity, because the second term in Eq. (15.2.19) is a constant, the change in kinetic energy in either reference frame is equal to 1 ΔK = µ v1, 2 2 − v1, 2 2 . (15.2.20) f i 2 (( ) ( )) This generalizes to any two relatively inertial reference frames because the relative velocity is a reference frame independent quantity, the change in kinetic energy is independent of the choice of relatively inertial reference frames. We showed in Appendix 13A that when two particles of masses m1 and m2 interact, the work done by the interaction force is equal to W= (( 1 µ v1, 2 2 2 ) − (v ) ) . 2 f 1, 2 i (15.2.21) Hence we explicitly verified that for our two-particle system W = ΔK sys . (15.2.22) 15-6 15.3 Characterizing Collisions In a collision, the ratio of the magnitudes of the initial and final relative velocities is called the coefficient of restitution and denoted by the symbol e , e= vB . vA (15.3.1) If the magnitude of the relative velocity does not change during a collision, e = 1, then the change in kinetic energy is zero, (Eq. (15.2.21)). Collisions in which there is no change in kinetic energy are called elastic collisions, ΔK = 0, elastic collision . (15.3.2) If the magnitude of the final relative velocity is less than the magnitude of the initial relative velocity, e < 1, then the change in kinetic energy is negative. Collisions in which the kinetic energy decreases are called inelastic collisions, ΔK < 0, inelastic collision . (15.3.3) If the two objects stick together after the collision, then the relative final velocity is zero, e = 0 . Such collisions are called totally inelastic. The change in kinetic energy can be found from Eq. (15.2.21), 1 1 m1m2 2 ΔK = − µ v 2A = − v , totally inelastic collision . 2 2 m1 + m2 A (15.3.4) If the magnitude of the final relative velocity is greater than the magnitude of the initial relative velocity, e > 1, then the change in kinetic energy is positive. Collisions in which the kinetic energy increases are called superelastic collisions, ΔK > 0, superelastic collision . (15.3.5) 15.4 One-Dimensional Collisions Between Two Objects 15.4.1 One Dimensional Elastic Collision in Laboratory Reference Frame Consider a one-dimensional elastic collision between two objects moving in the x direction. One object, with mass m1 and initial x -component of the velocity v1x,i , collides with an object of mass m2 and initial x -component of the velocity v2 x,i . The scalar components v1x,i and v1x,i can be positive, negative or zero. No forces other than the interaction force between the objects act during the collision. After the collision, the 15-7 final x -component of the velocities are v1x, f and v2 x, f . We call this reference frame the “laboratory reference frame”. Figure 15.5 One-dimensional elastic collision, laboratory reference frame For the collision depicted in Figure 15.5, v1x,i > 0 , v2 x,i < 0 , v1x, f < 0 , and v2 x, f > 0 . Because there are no external forces in the x -direction, momentum is constant in the x direction. Equating the momentum components before and after the collision gives the relation m1v1x, i + m2 v2 x, i = m1v1x, f + m2 v2 x, f . (15.4.1) Because the collision is elastic, kinetic energy is constant. Equating the kinetic energy before and after the collision gives the relation 1 1 1 1 2 2 m1v1x,i + m2 v22x,i = m1v1x, + m2 v22x, f f 2 2 2 2 (15.4.2) Rewrite these Eqs. (15.4.1) and (15.4.2) as m1 (v1x,i − v1x, f ) = m2 (v2 x, f − v2 x,i ) (15.4.3) 2 2 m1 (v1x,i − v1x, ) = m2 (v22x, f − v22x,i ) . f (15.4.4) Eq. (15.4.4) can be written as m1 (v1x,i − v1x, f )(v1x,i + v1x, f ) = m2 (v2 x, f − v2 x,i )(v2 x, f + v2 x,i ) . (15.4.5) Divide Eq. (15.4.4) by Eq. (15.4.3), yielding v1x,i + v1x, f = v2 x,i + v2 x, f . (15.4.6) v1x,i − v2 x,i = v2 x, f − v1x, f . (15.4.7) Eq. (15.4.6) may be rewritten as Recall that the relative velocity between the two objects is defined to be     v rel ≡ v1,2 ≡ v1 − v 2 . (15.4.8) 15-8 where we used the superscript “rel” to remind ourselves that the velocity is a relative velocity (and to simplify our notation). Thus vxrel,i = v1x,i − v2 x,i is the initial x -component of the relative velocity, and vxrel, f = v1x, f − v2 x, f is the final x -component of the relative velocity. Therefore Eq. (15.4.7) states that during the interaction the initial relative velocity is equal to the negative of the final relative velocity   v rel = −v relf , (1− dimensional energy-momentum prinicple) . i (15.4.9) Consequently the initial and final relative speeds are equal. We shall call this relationship between the relative initial and final velocities the one-dimensional energy-momentum principle because we have combined these two principles to realize this result. The energy-momentum principle is independent of the masses of the colliding particles. Although we derived this result explicitly, we have already shown that the change in kinetic energy for a two-particle interaction (Eq. (15.2.20)), in our simplified notation is given by 1 ΔK = µ ((v rel )2f − (v rel )2i ) (15.4.10) 2 Therefore for an elastic collision where ΔK = 0 , the square of the relative speed remains constant (v rel )2f = (v rel )2i . (15.4.11) For a one-dimensional collision, the magnitude of the relative speed remains constant but the direction changes by 180 . We can now solve for the final x -component of the velocities, v1x, f and v2 x, f , as follows. Eq. (15.4.7) may be rewritten as v2 x, f = v1x, f + v1x,i − v2 x,i . (15.4.12) Now substitute Eq. (15.4.12) into Eq. (15.4.1) yielding m1v1x,i + m2 v2 x,i = m1v1x, f + m2 (v1x, f + v1x,i − v2 x,i ) . (15.4.13) Solving Eq. (15.4.13) for v1x, f involves some algebra and yields v1x, f = m1 − m2 2 m2 v1x,i + v . m1 + m2 m1 + m2 2 x,i (15.4.14) 15-9 To find v2 x, f , rewrite Eq. (15.4.7) as v1x, f = v2 x, f − v1x,i + v2 x,i . (15.4.15) Now substitute Eq. (15.4.15) into Eq. (15.4.1) yielding m1v1x,i + m2 v2 x,i = m1 (v2 x, f − v1x,i + v2 x,i )v1x, f + m2 v2 x, f . (15.4.16) We can solve Eq. (15.4.16) for v2 x, f and determine that v2 x, f = v2 x,i m2 − m1 2 m1 . + v1x,i m2 + m1 m2 + m1 (15.4.17) Consider what happens in the limits m1 >> m2 in Eq. (15.4.14). Then v1x, f → v1x,i + 2 mv ; m1 2 2 x,i (15.4.18) the more massive object’s velocity component is only slightly changed by an amount proportional to the less massive object’s x -component of momentum. Similarly, the less massive object’s final velocity approaches v2 x, f → −v2 x,i + 2v1x,i = v1x,i + v1x,i − v2 x,i . (15.4.19) rel v2 x, f − v1x,i = v1x,i − v2 x,i = vx,i . (15.4.20) We can rewrite this as i.e. the less massive object “rebounds” with the same speed relative to the more massive object which barely changed its speed. If the objects are identical, or have the same mass, Eqs. (15.4.14) and (15.4.17) become v1x, f = v2 x,i , v2 x, f = v1x,i ; (15.4.21) the objects have exchanged x -components of velocities, and unless we could somehow distinguish the objects, we might not be able to tell if there was a collision at all. 15-10 15.4.2 One-Dimensional Collision Between Two Objects – Center-of-Mass Reference Frame We analyzed the one-dimensional elastic collision (Figure 15.5) in Section 15.4.1 in the laboratory reference frame. Now let’s view the collision from the center-of-mass (CM) frame. The x -component of velocity of the center-of-mass is vx,cm = m1 v1x,i + m2 v2 x,i m1 + m2 . (15.4.22) With respect to the center-of-mass, the x -components of the velocities of the objects are v1′x,i = v1x,i − vx,cm = (v1x,i − v2 x,i ) v2′ x,i = v2 x,i − vx,cm m2 m1 + m2 m1 = (v2 x,i − v1x,i ) . m1 + m2 (15.4.23) In the CM frame the momentum of the system is zero before the collision and hence the momentum of the system is zero after the collision. For an elastic collision, the only way for both momentum and kinetic energy to be the same before and after the collision is either the objects have the same velocity (a miss) or to reverse the direction of the velocities as shown in Figure 15.6. Figure 15.6 One-dimensional elastic collision in center-of-mass reference frame In the CM frame, the final x -components of the velocities are v1′x, f = −v1′x,i = (v2 x,i − v1x,i ) v2′ x, f m2 m1 + m2 m1 = −v2′ x,i = (v2 x,i − v1x,i ) . m1 + m2 (15.4.24) The final x -components of the velocities in the “laboratory frame” are then given by 15-11 v1x, f = v1′x, f + vx,cm = (v2 x,i − v1x,i ) = v1x,i m v + m2 v2 x,i m2 + 1 1x,i m1 + m2 m1 + m2 (15.4.25) m1 − m2 2 m2 + v2 x,i m1 + m2 m1 + m2 as in Eq. (15.4.14) and a similar calculation reproduces Eq. (15.4.17). 15.5 Worked Examples Example 15.1 Elastic One-Dimensional Collision Between Two Objects î î v1,i = v1,x,i î v 2,i = 0 1 2 v1, f = v1,x, f î 1 initial state m2 = 2m1 v 2, f = v2,x, f î final state m2 = 2m1 2 Figure 15.7 Elastic collision between two non-identical carts Consider the elastic collision of two carts along a track; the incident cart 1 has mass m1 and moves with initial speed v1,i . The target cart has mass m2 = 2 m1 and is initially at rest, v2,i = 0 , (Figure 15.7). Immediately after the collision, the incident cart has final speed v1, f and the target cart has final speed v2, f . Calculate the final x -component of the velocities of the carts as a function of the initial speed v1,i . Solution The momentum flow diagram for the objects before (initial state) and after (final state) the collision are shown in Figure 15.7. We can immediately use our results above with m2 = 2 m1 and v2,i = 0 . The final x -component of velocity of cart 1 is given by Eq. (15.4.14), where we use v1x,i = v1,i 15-12 1 v1x, f = − v1,i . 3 (15.5.1) The final x -component of velocity of cart 2 is given by Eq. (15.4.17) v2 x, f = 2 v . 3 1,i (15.5.2) Example 15.2 The Dissipation of Kinetic Energy in a Completely Inelastic Collision Between Two Objects î î v1,i v 2,i = 0 1 2 initial state vf final state 1 2 Figure 15.7b Inelastic collision between two non-identical carts An incident cart of mass m1 and initial speed v1, i collides completely inelastically with a cart of mass m2 that is initially at rest (Figure 15.7b). There are no external forces acting on the objects in the direction of the collision. Find ΔK / K initial = (K final − K initial ) / K initial . Solution: In the absence of any net force on the system consisting of the two carts, the momentum after the collision will be the same as before the collision. After the collision the carts will move in the direction of the initial velocity of the incident cart with a common speed v f found from applying the momentum condition m1v1, i = (m1 + m2 )v f ⇒ vf = m1 v1, i . m1 + m2 (15.5.3) The initial relative speed is virel = v1, i . The final relative velocity is zero because the carts stick together so using Eq. (15.3.4), the change in kinetic energy is 1 m1m2 2 1 ΔK = − µ (virel )2 = − v1, i . 2 2 m1 + m2 (15.5.4) 15-13 The ratio of the change in kinetic energy to the initial kinetic energy is then ΔK / K initial = − m2 . m1 + m2 (15.5.5) As a check, we can calculate the change in kinetic energy via 1 1 ΔK = (K f − K i ) = (m1 + m2 )v 2f − v1,2 i 2 2 2 ⎛ m1 ⎞ 2 1 2 1 = (m1 + m2 ) ⎜ v1, i − v1, i 2 2 ⎝ m1 + m2 ⎟⎠ (15.5.6) ⎛ m1 ⎞⎛1 1 m1m2 2 ⎞ =⎜ − 1⎟ ⎜ m1v1,2 i ⎟ = − v1, i . ⎠ 2 m1 + m2 ⎝ m1 + m2 ⎠ ⎝ 2 in agreement with Eq. (15.5.4). Example 15.3 Bouncing Superballs 1 2 g M 2 >> M1 Figure 15.8b Two superballs dropping Consider two balls that are dropped from a height hi above the ground, one on top of the other (Figure 15.8). Ball 1 is on top and has mass M1 , and ball 2 is underneath and has mass M 2 with M 2 >> M1 . Assume that there is no loss of kinetic energy during all collisions. Ball 2 first collides with the ground and rebounds. Then, as ball 2`starts to move upward, it collides with the ball 1 which is still moving downwards (figure below left). How high will ball 1 rebound in the air? Hint: consider this collision as seen by an observer moving upward with the same speed as the ball 2 has after it collides with ground. What speed does ball 1 have in this reference frame after it collides with the ball 2? 15-14 Solution The system consists of the two balls and the earth. There are five special states for this motion shown in the figure below. part a) Initial State: the balls are released from rest at a height hi above the ground. State A: the balls just reach the ground with speed va = 2ghi . This follows from ΔEmech = 0 ⇒ ΔK = −ΔU . Thus (1 / 2)mva2 − 0 = −mgΔh = mghi ⇒ va = 2ghi . State B: immediately before the collision of the balls. Ball 2 has collided with the ground and reversed direction with the same speed, va , but ball 1 is still moving downward with speed va . State C: immediately after the collision of the balls. Because we are assuming that m2 >> m1 , ball 2 does not change its speed as a result of the collision so it is still moving upward with speed va . As a result of the collision, ball 1 moves upward with speed vb . Final State: ball 1 reaches a maximum height h f = vb 2 / 2g above the ground. This again follows from ΔK = −ΔU ⇒ 0 − (1 / 2)mvb2 = −mgΔh = −mgh f ⇒ h f = vb2 / 2g . Choice of Reference Frame: As indicated in the hint above, this collision is best analyzed from the reference frame of an observer moving upward with speed va , the speed of ball 2 just after it rebounded with 15-15 the ground. In this frame immediately, before the collision, ball 1 is moving downward with a speed vb′ that is twice the speed seen by an observer at rest on the ground (lab reference frame). va′ = 2 va (15.5.7) The mass of ball 2 is much larger than the mass of ball 1, m2 >> m1 . This enables us to consider the collision (between States B and C) to be equivalent to ball 1 bouncing off a hard wall, while ball 2 experiences virtually no recoil. Hence ball 2 remains at rest in the reference frame moving upwards with speed va with respect to observer at rest on ground. Before the collision, ball 1 has speed va′ = 2 va . Since there is no loss of kinetic energy during the collision, the result of the collision is that ball 1 changes direction but maintains the same speed, vb′ = 2 va . (15.5.8) However, according to an observer at rest on the ground, after the collision ball 1 is moving upwards with speed vb = 2 va + va = 3va . (15.5.9) While rebounding, the mechanical energy of the smaller superball is constant (we consider the smaller superball and the Earth as a system) hence between State C and the Final State, ΔK + ΔU = 0 . (15.5.10) 1 ΔK = − m1 (3va )2 . 2 (15.5.11) ΔU = m1 g h f . (15.5.12) The change in kinetic energy is The change in potential energy is So the condition that mechanical energy is constant (Equation (15.5.10)) is now 1 − m1 (3v1a )2 + m1 g h f = 0 . 2 (15.5.13) We can rewrite Equation (15.5.13) as 1 m1 g h f = 9 m1 ( va )2 . 2 (15.5.14) 15-16 Recall that we can also use the fact that the mechanical energy doesn’t change between the Initial State and State A yielding an equation similar to Eq. (15.5.14), m1 g hi = 1 m ( v )2 . 2 1 a (15.5.15) Now substitute the expression for the kinetic energy in Eq. (15.5.15) into Eq. (15.5.14) yielding m1 g h f = 9 m1 g hi . (15.5.16) Thus ball 1 reaches a maximum height h f = 9 hi . (15.5.17) 15.6 Two Dimensional Elastic Collisions 15.6.1 Two-dimensional Elastic Collision in Laboratory Reference Frame Consider the elastic collision between two particles in which we neglect any external forces on the system consisting of the two particles. Particle 1 of mass m1 is initially  moving with velocity v1, i and collides elastically with a particle 2 of mass m2 that is initially at rest. We shall refer to the reference frame in which one particle is at rest, ‘the target’, as the laboratory reference frame. After the collision particle 1 moves with   velocity v1, f and particle 2 moves with velocity v 2, f , (Figure 15.9). The angles θ1, f and θ 2, f that the particles make with the positive forward direction of particle 1 are called the laboratory scattering angles. v1, f 1 1 v1, i 1, f 2 2 2, f v 2, f Figure 15.9 Two-dimensional collision in laboratory reference frame  Generally the initial velocity v1, i of particle 1 is known and we would like to determine   the final velocities v1, f and v 2, f , which requires finding the magnitudes and directions 15-17 of each of these vectors, v1, f , v2, f , θ1, f , and θ 2, f . These quantities are related by the two equations describing the constancy of momentum, and the one equation describing constancy of the kinetic energy. Therefore there is one degree of freedom that we must specify in order to determine the outcome of the collision. In what follows we shall express our results for v1, f , v2, f , and θ 2, f in terms of v1, i and θ1, f .    = m1v1,i + m2 v 2,i in the initial state are given The components of the total momentum psys i by sys px,i = m1v1,i p sys = 0. y,i (15.6.1)    = m1v1, f + m2 v 2, f in the final state are given by The components of the momentum psys f px,sysf = m1 v1, f cosθ1, f + m2 v2, f cosθ 2, f p sys = m1 v1, f sin θ1, f − m2 v2, f sin θ 2, f . y, f (15.6.2) There are no any external forces acting on the system, so each component of the total momentum remains constant during the collision, pxsys,i = pxsys, f (15.6.3) p sys = p sys . y,i y, f (15.6.4) m1 v1,i = m1 v1, f cosθ1, f + m2 v2, f cosθ 2, f , (15.6.5) 0 = m1 v1, f sin θ1, f − m2 v2, f sin θ 2, f . (15.6.6) Eqs. (15.6.3) and (15.6.4) become The collision is elastic and therefore the system kinetic energy of is constant K i sys = K f sys . (15.6.7) Using the given information, Eq. (15.6.7) becomes 1 1 1 2 m1v1,i = m1v1,2 f + m2 v2,2 f . 2 2 2 (15.6.8) Rewrite the expressions in Eqs. (15.6.5) and (15.6.6) as m2 v2, f cosθ 2, f = m1 (v1,i − v1, f cosθ1, f ), (15.6.9) 15-18 m2 v2, f sin θ 2, f = m1v1, f sin θ1, f . (15.6.10) Square each of the expressions in Eqs. (15.6.9) and (15.6.10), add them together and use the identity cos 2 θ + sin 2 θ = 1 yielding v 2 2, f m12 2 = 2 (v1,i − 2v1,i v1, f cosθ1, f + v1,2 f ) . m2 (15.6.11) Substituting Eq. (15.6.11) into Eq. (15.6.8) yields 1 1 1 m12 2 2 2 m1v1,i = m1v1, f + (v1,i − 2v1,i v1, f cosθ1, f + v1,2 f ) . 2 2 2 m2 (15.6.12) Eq. (15.6.12) simplifies to ⎛ ⎛ m⎞ m m⎞ 2 , 0 = ⎜ 1+ 1 ⎟ v1,2 f − 1 2v1,i v1, f cosθ1, f − ⎜ 1− 1 ⎟ v1,i m2 ⎝ m2 ⎠ ⎝ m2 ⎠ (15.6.13) Let α = m1 / m2 then Eq. (15.6.13) can be written as 0 = (1+ α )v1,2 f − 2α v1,i v1, f cosθ1, f − (1− α )v1,2 i , (15.6.14) The solution to this quadratic equation is given by v1, f = ( 2 2 α v1,i cosθ1, f ± α 2 v1,i cos 2 θ1, f + (1− α 2 )v1,i (1+ α ) ) 1/2 . (15.6.15) Divide Eq. (15.6.10) by Eq. (15.6.9): v2, f sin θ 2, f v2, f cosθ 2, f = v1, f sin θ1, f v1,i − v1, f cosθ1, f . (15.6.16) Eq. (15.6.16) simplifies to tan θ 2, f = v1, f sin θ1, f v1,i − v1, f cosθ1, f . (15.6.17) The relationship between the scattering angles in Eq. (15.6.17) is independent of the masses of the colliding particles. Thus the scattering angle for particle 2 is 15-19 ⎛ v1, f sin θ1, f ⎞ θ 2, f = tan −1 ⎜ ⎟ ⎝ v1,i − v1, f cosθ1, f ⎠ (15.6.18) We can now use Eq. (15.6.10) to find an expression for the final velocity of particle 2 v2, f = α v1, f sin θ1, f sin θ 2, f . (15.6.19) Example 15.5 Elastic Two-dimensional collision of identical particles v1, f ˆj ˆi 1 1 v1, i 1, f 2 = 30 2, f 2 v 2, f Figure 15.10 Momentum flow diagram for two-dimensional elastic collision Object 1 with mass m1 is initially moving with a speed v1,i = 3.0m ⋅s −1 and collides elastically with object 2 that has the same mass, m2 = m1 , and is initially at rest. After the collision, object 1 moves with an unknown speed v1, f at an angle θ1, f with respect to its initial direction of motion and object 2 moves with an unknown speed v2, f , at an unknown angle θ 2, f (as shown in the Figure 15.10). Find the final speeds of each of the objects and the angle θ 2, f . Solution: Because the masses are equal, α = 1 . We are given that v1,i = 3.0 m ⋅s −1 and θ1, f = 30o . Hence Eq. (15.6.14) reduces to v1, f = v1,i cosθ1, f = (3.0 m ⋅s −1 )cos30 = 2.6 m ⋅s −1 . (15.6.20) Substituting Eq. (15.6.20) in Eq. (15.6.17) yields 15-20 ⎛ v1, f sin θ1, f ⎞ θ 2, f = tan −1 ⎜ ⎟ ⎝ v1,i − v1, f cosθ1, f ⎠ θ 2, f ⎛ ⎞ (2.6 m ⋅s −1 )sin(30 ) = tan ⎜ −1 −1  ⎝ 3.0 m ⋅s − (2.6 m ⋅s )cos(30 ) ⎟⎠ −1 (15.6.21) = 60. The above results for v1, f and θ 2, f may be substituted into either of the expressions in Eq. (15.6.9), or Eq. (15.6.11), to find v2, f = 1.5m ⋅ s −1 . Eq. (15.6.11) also has the solution v2, f = 0 , which would correspond to the incident particle missing the target completely. Before going on, the fact that θ1, f + θ 2, f = 90 , that is, the objects move away from the collision point at right angles, is not a coincidence. A vector derivation is presented in Example 15.6. We can see this result algebraically from the above result. Substituting Eq. (15.6.20) v1, f = v1,i cosθ1, f in Eq. (15.6.17) yields tan θ 2, f = cosθ1, f sin θ1, f 1− cosθ 2 1, f = cot θ1, f = tan(90 − θ1, f ) ; (15.6.22) showing that θ1, f + θ 2, f = 90 , the angles θ1, f and θ 2, f are complements. Example 15.6 Two-dimensional elastic collision between particles of equal mass Show that the equal mass particles emerge from a two-dimensional elastic collision at right angles by making explicit use of the fact that momentum is a vector quantity. v1, f ˆj ˆi 1 1 v1, i 1, f 2 2, f 2 v 2, f Figure 15.11 Elastic scattering of identical particles 15-21 Solution: Choose a reference frame in which particle 2 is initially at rest (Figure 15.11). There are no external forces acting on the two objects during the collision (the collision forces are all internal), therefore momentum is constant which becomes Eq. (15.6.24) simplifies to   psys = psys , i f (15.6.23)    m1v1, i = m1v1, f + m1v 2, f . (15.6.24)    v1,i = v1, f + v 2, f . (15.6.25) Recall the vector identity that the square of the speed is given by the dot product   v ⋅ v = v 2 . With this identity in mind, we take the dot product of each side of Eq. (15.6.25) with itself,       v1,i ⋅ v1,i = ( v1, f + v 2, f ) ⋅( v1, f + v 2, f ) (15.6.26)       = v1, f ⋅ v1, f + 2 v1, f ⋅ v 2, f + v 2, f ⋅ v 2, f . This becomes   2 v1,i = v1,2 f + 2 v1, f ⋅ v 2, f + v2,2 f . (15.6.27) Recall that kinetic energy is the same before and after an elastic collision, and the masses of the two objects are equal, so constancy of energy, (Eq. (15.4.2)) simplifies to 2 v1,i = v1,2 f + v2,2 f . (15.6.28) Comparing Eq. (15.6.27) to Eq. (15.6.28), we see that   v1, f ⋅ v 2, f = 0 . (15.6.29) The dot product of two nonzero vectors is zero when the two vectors are at right angles to each other justifying our claim that the collision particles emerge at right angles to each other. Example 15.7 Two dimensional collision between particles of unequal mass Particle 1 of mass m1 , initially moving in the positive x -direction (to the right in the figure below) with speed v1,i , collides with particle 2 of mass m2 = m1 / 3 , which is initially moving in the opposite direction (Figure 15.12) with an unknown speed v2,i . Assume that the total external force acting on the particles is zero. Do not assume the collision is elastic. After the collision, particle 1 moves with speed v1, f = v1,i / 2 in the negative y -direction. After the collision, particle 2 moves with an unknown speed v2, f , 15-22 at an angle θ 2, f = 45o with respect to the positive x -direction. (i) Determine the initial speed v2,i of particle 2 and the final speed v2, f of particle 2 in terms of v1,i . (ii) Is the collision elastic? before after 1 v1,i v2, f 2 v2,i 2 ĵ î = 45 m2 = m / 3 m1 = m 1 v1, f = v1,i / 2 Figure 15.12 Two-dimensional collision between particles of unequal mass Solution: We choose as our system the two particles. We are given that v1, f = v1,i / 2 . We apply the two momentum conditions, m1 v1,i − (m1 / 3)v2,i = (m1 / 3) v2, f ( 2 / 2) (15.6.30) 0 = m1 v1, f − (m1 / 3) v2, f ( 2 / 2) . (15.6.31) Solve Eq. (15.6.31) for v2, f v2, f = 3 2v1, f = 3 2 v 2 1,i (15.6.32) Substitute Eq. (15.6.32) into Eq. (15.6.30) and solve for v2,i v2,i = (3 / 2)v1,i . (15.6.33) The initial kinetic energy is then 1 1 7 2 2 2 m1v1,i + (m1 / 3)v2,i = m1v1,i . 2 2 8 (15.6.34) 1 1 1 3 7 2 2 2 m1v1,2 f + m2 v2,2 f = m1v1,i + m1v1,i = m1v1,i . 2 2 8 4 8 (15.6.35) Ki = The final kinetic energy is Kf = Comparing our results, we see that kinetic energy is constant so the collision is elastic. 15-23 15.7 Two-Dimensional Collisions in Center-of-Mass Reference Frame 15.7.1 Two-Dimensional Collision in Center-of-Mass Reference Frame Consider the elastic collision between two particles in the laboratory reference frame  (Figure 15.9). Particle 1 of mass m1 is initially moving with velocity v1, i and collides elastically with a particle 2 of mass m2 that is initially at rest. After the collision the   particle 1 moves with velocity v1, f and particle 2 moves with velocity v 2, f . In section 15.7.1 we determined how to find v1, f , v2, f , and θ 2, f in terms of v1, i and θ 2, f . We shall now analyze the collision in the center-of-mass reference frame, which is boosted form the laboratory frame by the velocity of center-of-mass given by  m1v1, i  . v cm = m1 + m2 (15.6.36) Because we assumed that there are no external forces acting on the system, the center-ofmass velocity remains constant during the interaction. v1, f 1 v1,i 1 cm 2 v 2, f v 2,i 2 Figure 15.13 Two-dimensional elastic collision in center-of-mass reference frame Recall the velocities of particles 1 and 2 in the center-of-mass frame are given by (Eq.,(15.2.9) and (15.2.10)). In the center-of-mass reference frame the velocities of the two incoming particles are in opposite directions, as are the velocities of the two outgoing particles after the collision (Figure 15.13). The angle Θ cm between the incoming and outgoing velocities is called the center-of-mass scattering angle. 15-24 15.7.2 Scattering in the Center-of-Mass Reference Frame  Consider a collision between particle 1 of mass m1 and velocity v1,i and particle 2 of mass m2 at rest in the laboratory frame. Particle 1 is scattered elastically through a scattering angle Θ in the center-of-mass frame. The center-of-mass velocity is given by  m1v1,i  . v cm = m1 + m2 (15.6.37) In the center-of-mass frame, the momentum of the system of two particles is zero      0 = m1v1,′ i + m2 v′2,i = m1v1,′ f + m2 v′2, f . (15.6.38) m   v1,′ i = − 2 v′2,i . m1 (15.6.39) m   v1,′ f = − 2 v′2, f m1 (15.6.40) Therefore The energy condition in the center-of-mass frame is 1 1 1 1 m1v1,′ 2i + m2 v2,′ 2i = m1v1,′ 2f + m2 v2,′ 2f . 2 2 2 2 (15.6.41) Substituting Eqs. (15.6.39) and (15.6.40) into Eq. (15.6.41) yields v1,′ i = v1,′ f . (15.6.42) (we are only considering magnitudes). Therefore v2,′ i = v2,′ f . (15.6.43) Because the magnitude of the velocity of a particle in the center-of-mass reference frame is proportional to the relative velocity of the two particles, Eqs. (15.6.42) and (15.6.43) imply that the magnitude of the relative velocity also does not change   v1,′ 2, i = v1,′ 2, f , (15.6.44) verifying our earlier result that for an elastic collision the relative speed remains the same, (Eq. (15.2.20)). However the direction of the relative velocity is rotated by the center-of-mass scattering angle Θ cm . This generalizes the energy-momentum principle to two dimensions. Recall that the relative velocity is independent of the reference frame, 15-25     v1, i − v 2, i = v1,′ i − v′2, i (15.6.45)   In the laboratory reference frame v 2,i = 0 , hence the initial relative velocity is    v1,′ 2, i = v1, 2, i = v1, i , and the velocities in the center-of-mass frame of the particles are then µ   v1,′ i = v1, i m1 µ   v′2, i = − v1, i m2 (15.6.46) . (15.6.47) Therefore the magnitudes of the final velocities in the center-of-mass frame are v1,′ f = v1,′ i = µ µ µ v1,′ 2, i = v1, 2, i = v1, i . m1 m1 m1 (15.6.48) v2,′ f = v2,′ i = µ µ µ v1,′ 2, i = v1, 2, i = v . m2 m2 m2 1, i (15.6.49) Example 15.8 Scattering in the Lab and CM Frames  Particle 1 of mass m1 and velocity v1,i by a particle of mass m2 at rest in the laboratory frame is scattered elastically through a scattering angle Θ in the center of mass frame, (Figure 15.14). Find (i) the scattering angle of the incoming particle in the laboratory frame, (ii) the magnitude of the final velocity of the incoming particle in the laboratory reference frame, and (iii) the fractional loss of kinetic energy of the incoming particle. ˆi 1 v1, f v1, f ˆj 1 1 v1, i v1,i 1, f 2 cm 1 2, f cm 2 2 v 2,i 2 v 2, f v 2, f Figure 15.14 Scattering in the laboratory and center-of-mass reference frames 15-26 Solution: i) In order to determine the center-of-mass scattering angle we use the transformation law for velocities    v1,′ f = v1, f − v cm . (15.6.50) In Figure 15.15 we show the collision in the center-of-mass frame along with the laboratory frame final velocities and scattering angles. v1, f v1, f 1, f 1 1 ˆj ˆi v cm cm v1,i cm v 2,i 2 v cm v 2, f 2 2, f v 2, f Figure 15.15 Final velocities of colliding particles Vector decomposition of Eq. (15.6.50) yields v1, f cosθ1, i = v1,′ f cosΘ cm − vcm , (15.6.51) v1, f sin θ1, i = v1,′ f sinΘ cm . (15.6.52) where we choose as our directions the horizontal and vertical Divide Eq. (15.6.52) by (15.6.51) yields v sin θ1, i v1,′ f sinΘ cm (15.6.53) tanθ1, i = 1, f = v1, f cosθ1, i v1,′ f cosΘ cm − vcm Because v1,′ i = v1,′ f , we can rewrite Eq. (15.6.53) as tanθ1, i = v1,′ i sinΘ cm v1,′ i cosΘ cm − vcm (15.6.54) We now substitute Eqs. (15.6.48) and vcm = m1v1, i / (m1 + m2 ) into Eq. (15.6.54) yielding 15-27 tanθ1, i = m2 sinΘ cm . cosΘ cm − m1 / m2 (15.6.55) Thus in the laboratory frame particle 1 scatters by an angle ⎛ m2 sinΘ cm ⎞ θ1, i = tan −1 ⎜ ⎟ . ⎝ cosΘ cm − m1 / m2 ⎠ (15.6.56) ii) We can calculate the square of the final velocity in the laboratory frame       v1, f ⋅ v1, f = ( v1,′ f + v cm ) ⋅( v1,′ f + v cm ) . (15.6.57)   v1, f 2 = v1,′ f 2 + 2v1,′ f ⋅ v cm + vcm 2 = v1,′ f 2 + 2v1,′ f vcm cosΘ cm + vcm 2 . (15.6.58) which becomes We use the fact that v1,′ f = v1,′ i = ( µ / m1 )v1,2, i = ( µ / m1 )v1, i = (m2 / m1 + m2 )v1, i to rewrite Eq. (15.6.58) as 2 v1, f 2 ⎛ m2 ⎞ m2 m1 m12 2 =⎜ v1, i + 2 v cosΘ cm + v 2 . 2 1, i 2 1, i ⎟ (m1 + m2 ) (m1 + m2 ) ⎝ m1 + m2 ⎠ Thus v1, f (m = 2 2 + 2m2 m1 cosΘ cm + m12 m1 + m2 ) (15.6.59) 1/2 v1, i . (15.6.60) (iii) The fractional change in the kinetic energy of particle 1 in the laboratory frame is given by K1, f − K1, i K1, i = v1, f 2 − v1, i 2 v1, i 2 m2 2 + 2m2 m1 cosΘ cm + m12 2m2 m1 (cosΘ cm − 1) .(15.6.61) = −1= 2 (m1 + m2 ) (m1 + m2 )2 We can also determine the scattering angle Θ cm in the center-of-mass reference frame from the scattering angle θ1, i of particle 1 in the laboratory. We now rewrite the momentum relations as v1, f cosθ1, i + vcm = v1,′ f cosΘ cm , (15.6.62) v1, f sin θ1, i = v1,′ f sinΘ cm . (15.6.63) In a similar fashion to the above argument, we have that 15-28 tanΘ cm = v1, f sin θ1, f v1, f cosθ1, f + vcm . (15.6.64) Recall from our analysis of the collision in the laboratory frame that if we specify one of the four parameters v1, f , v2, f , θ1, f , or v1, f , then we can solve for the other three in terms of the initial parameters v1, i and v2, i . With that caveat, we can use Eq. (15.6.64) to determine Θ cm . 15-29