Consider the collision of two particles, each of mass mo. In experiment A, a particle moving at 0.9cstrikes a stationary particle.

  1. What is the total kinetic energy before the collision?
  2. In experiment B, both particles are moving at a speed u(relative to the lab), directly towards one another. If the total kinetic energy before the collision in experiment B is the same as that in experiment A, what is u?
  3. In both particles, the particles stick together. Find the mass of the resulting single particle in each experiment. In which is more of the initial kinetic energy converted to mass?

Short Answer

Expert verified

a) In experiment A, the total kinetic energy before the collision is.1.29moc2

b) The final mass of the particle after the collision is2.55mo.

c) In experiment B, the speed of both the particles is0.794c. The final mass of the particle after the collision is.3.26mo

Step by step solution

01

Determine total kinetic energy before collision in experiment A

In this problem, two experiments of inelastic collision are performed. In experiment A, a particle moving at 0.9cstrikes a stationary particle and two particles stick together. Let us calculate the initial kinetic energy of the system.

KEinitial=(γ0.9c1)moc2+(γ0c1)moc2

Here, for particle 1, the Lorentz factor will be 2.29, and for particle 2, the Lorentz factor will be one as the velocity is zero. Putting these values in the above equation, we get the initial kinetic energy as follows:

.KEinitial=1.29moc2

02

Determine total kinetic energy before collision in experiment B

In experiment B, two particles are coming at each other at velocity u.The total energy before the collision in this experiment is the same as the initial kinetic energy in experiment A. Let us calculate the velocity u from the above information.

KEB=KEA(γu1)moc2+(γu1)moc2=1.29moc22(γu1)=1.29γu=1.645

Using Lorentz formula to calculate speed,

11-u2c2=1.645u=c1-11.6452u=0.794c

03

Apply energy and momentum conservation for both experiments

in both experiments, the total kinetic energy before the collision is equal.The total kinetic energy after the collision can be calculated using the final mass at the end of both the experiments. So,for experiment A,

momentum conserved:

.γ0.9cmo(0.9c)+0=γfmfufγfmfuf=2.06moc

energy conserved: .

γ0.9cmoc2+moc2=γfmfc2γfmf=3.29mo

Dividing the both resulting conserved equations,

.uf=0.6353c

And using this value for velocity, one can find the corresponding Lorentz factor asγf=1.29. Then putting this value in energy conserved equation,

mf=2.55mo

Now, in experiment B, applying energy conservation,

.γ0.79cmoc2+γ0.79cmoc2=γfmfc2

Here, γf=1because the final velocity will be zero.

localid="1659091830810" mf=2γ0.79cmo=211(0.79)2mo=3.26mo

As you can see in both experiments, mass increases after the collision. This implies that the total kinetic energy of the system in both experiments decreases, increasing mass. In experiment B, the change in mass is more than that in experiment A. Therefore, more initial kinetic energy will be converted to mass in experiment B.

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Most popular questions from this chapter

Anna and Bob are In identical spaceships, each 100 m long. The diagram shows Bob's, view as Anna's ship passes at 0.8c. Just as the backs of the ships pass one another, both clocks.there read O. At the instant shown, Bob Jr., on board Bob's ship, is aligned with the very front of Anna's ship. He peers through a window in Anna's ship and looks at the clock. (a) In relation to his own ship, where is Bob Jr? (b) What does the clock he sees read?

Question: Equation (2-38) show that four-momentum of a particle obeys a Lorentz transformation. If we sum momentum and energy over all particles in a system, we see that the total momentum and energy also constitute a four-vector. It follows that (Etotal/c)2-Ptotal2 is the same quantity in any frame of reference. Depending on what is known, this can be a quicker route to solving problems than writing out momentum and energy conservation equations. In the laboratory frame, a particle of mass m and energy Ei collide with another particle of mass initially stationary, forming a single object of mass . (a) Determine the frame of reference where the after-collision situation is as simple as possible, then determine the invariant in that frame. (b) Calculate the invariant before the collision in the laboratory frame in terms of M and Ei . (You will need to use Ei2/c2-p2=m2c2 for the initially moving particle to eliminate its momentum.) Obtain an expression for M in terms of m and Ei . (c) Write out momentum and energy conservation in the laboratory frame, using uf for the speed of the initially moving particle and for the speed of the final combined particle. Show that they give the same result for M in terms of m and Ei. (Note: The identity γu2u2=γu2c2-c2 will be very handy.)

Equations (2-38) relate momentum and total energy in two frames. Show that they make sense in the non-relativistic limit.

Consider Anna, Bob and Carl in the twin paradox.

(a) According to Anna, when Planet X passes her, clocks on Planet X and Earth tick simultaneously. What is the time interval between these two events in the Earth-Planet X frame?

(b) According to Carl, when Planet X passes, clocks on Planet X and Earth tick simultaneously. What is the time interval between these two events in the Earth-Planet X frame?

(c) What does the clock on Planet X read when Carl and Anna reach it? Show how your results from part (a) and (b) agree with Figure 2.20.

From p=γumu (i.e., px=γumux,py=γumuy and pz=γumuz ), the relativistic velocity transformation (2-20), and the identity γu'=(1-uxv/c2)γvγu show that py'=py and pz'=pz.

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