Special Relativity: Dynamics
Energy and Momentum
In this setion we will turn to a discussion of some interesting aspects of Special Relativity, concerning how particle and objects gain motion, and how they interact. In this section we will arrive at an expression that looks something like the definition of momentum, and seems to be a conserved quantity under the new rules of Special Relativity. With this in mind consider the following setup.
If the y -velocity is much greater than the x -velocity, then particle A is essentially at rest with respect to particle B in A's frame. Time dilation tells us that particle B's clock must be running slow by a factor . Particle B's clock ticks once for every vertical line crossed (independent of frame), so particle B must be moving more slowly than A in the x -direction by a factor . Thus the magnitudes of the x -velocities of the particles are not the same. This means that the Newtonian p x = mv x is not a conserved quantity because the momentum of particle B would be smaller than the momentum of particle A by the factor 1/γ since | v x| is larger for particle A. We have shown that if momentum is to be conserved, the momenta of A and B better be the same. However, the solution to the difficulty is not so hard: we define momentum as:
|p x = γmv x =|
A is at rest in the y -direction so γ A = 1 , and mv x = γmv x . For B however, this we have exactly taken care of the problem: the factor by which particle B's speed was smaller is canceled out by the γ so particle B also has momentum p x = = mv x .
In three dimensions the equation for relativistic momentum becomes:
We have not shown here that γmv is conserved--this is the job of experiments. What we have done is to provide some motivation for the equation for relativistic momentum by showing that γm (or some constant multiple of it) is the only vector of this form which has any chance of being conserved in a collision (for instance, γ 2 m we now know, is certainly not conserved).
To develop a concept of relativistic energy we will again consider a scenario and show that a particular expression is conserved. This expression we just happen to give the label 'energy.'
|γ v mv + 0 = γMuâám = âáM =|
Surprisingly, M is not equal to 2m , but is larger by a factor γ . However, in the limit u < < c , M 2m as expected from the correspondence principle.
Let us now state the expression for relativistic energy and check whether it is conserved:
If γmc 2 is conserved then:
|γ v mc 2 +1×mc 2||=||γ u Mc 2âá m + m|
This last equality is clearly true. Thus we have found a quantity that looks a little bit like classical energy and is conserved in collisions. What happens in the limit v < < c ? We can use the binomial series expansion to expand (1 - v 2/c 2)-1/2 as follows:
|EâÉáγmc 2||=||1 - v 2/c 2)-1/2|
|=||mc 2 1 + + +|
|=||mc 2 + mv 2 +|
The higher order terms can be neglected for v < < c . First note that for v = 0 the second (and all higher) terms are zero so we have the famous E = mc 2 for a particle at rest. Second, mc 2 is just a constant so conservation of energy reduces to the conservation of mv 2/2 in this limit. Moreover, the reduction of E = γmc 2 to the Newtonian form in this limit justifies our choice of γmc 2 rather that say, 5γmc 8 as our expression for energy.
Energy and Momentum
Note that when we used the term 'energy' we mean γmc 2 , which is a particle's total energy. The particle's 'kinetic energy', however, is the excess energy due to its motion, over and above the energy it has when at rest: KE = γmc 2 - mc 2 . Thus any particle has an amount of energy mc 2 when at rest; this is the famous mass-energy relationship which explains the energy release in many nuclear reactions, and explains, for example, why all stable nuclei have a mass that is less than their constituent particles. Because of this kinetic energy is not always conserved it a collision or decay: it is the total energy γmc 2 , as we have seen, that is conserved.
There is also an extremely important relationship between energy and momentum:
|E 2 - ||
|= γ 2 m 2 c 4 1 -|
|= m 2 c 4|
Since m 2 c 4 is a constant, independent of reference frame, the quantity E 2 - | must also be frame invariant (the same in every inertial frame). Another important relation is that = .
The above equation suggests that there is a special relationship between energy and momentum. Consider a frame F' moving with speed v with respect to frame F along their mutual x / x' -direction (just like when we derived the Lorentz transformations). There is a particle in F' that has energy E' and momentum p' (and is moving also in the x -direction). What is E and p in the frame F ? The answer looks very familiar:
|ΔE = γ v(ΔE' + vΔp')|
|Δp = γ v(Δp' + vΔE'/c 2)|
γ v is the γ factor associated with the relative speed between the frames ( v ). Not surprisingly these transformations look precisely like the Lorentz transformations between space and time in different frames. These equations also hold if E and p represent total energy and total momentum of a system of particles. Moreover they make it clear that if E and p are conserved in one frame, then they are conserved in any other inertial frame; this is very important to make the conservation laws we derived above meaningful. This arises just because E and p in one frame must be linear functions of E' and p' in another frame. Since the latter quantities are both conserved any linear function of them must be conserved also. Note that, just as with the spacetime transformations the above applies only to the x -direction (there is nothing special about x , except that we have arbitrarily chosen it to be our direction of motion) and p y = p y' and p z = p z' .
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