Relativity in brief... or in detail..

Where does E = mc2 come from? Energy in Newtonian mechanics and in relativity

Under relativity, the laws of physics may be the same for two observers with relative motion, but they sometimes look unfamiliar to those of us who are used to putting kinetic energy = ½mv2. In this animation, a rocket engine does work at a constant rate, ie it produces constant power. (This is not the usual behaviour or rockets, but it means that we can see what increasing the kinetic energy does to speed and momentum under classical and relativistic mechanics.) We discuss this animation further below.

Another way of writing Newton's second law in classical mechanics is the work energy theorem. By integrating the resultant force F that acts on a body with respect to the distance over which the centre of mass moves, one obtains the important result that the work done by F equals the change in the quantity ½mv2, a quantity that we call the kinetic energy. That's the theorem. As you might expect, things are a bit more complicated in relativity. Let's start with Newton's second law, that states the force is equal to the time rate of change in momentum:

We integrate to get the work done:
Now we need some expressions to do the substitutions:
We need to integrate with respect to both v and γ, so it's helpful to write:
and substitution in our integrand gives:
From here we get the expression for the kinetic energy, K, in Special Relativity:
graph of total energy, proper plus kinetic This is a very important expression, so we should check that, at low speeds, it corresponds to the classical expression. Using the expansion valid for small v/c:
as shown in the graph at right - the purple line is ½mv2+mc2. Ah, that's reassuring. But it also shows us Einstein's speed limit. In the classical expression, v is proportional to the square root of K. In principle, v could be as large as one liked. In relativistic mechanics, however, (γ - 1) increases linearly with the kinetic energy. And γ goes to infinity as v goes to c. A finite amount of energy can never accelerate a body to the speed of light.

So now let's look at equation (*) again:

Where did the 1 on the right hand side come from? It's the starting value of the integral. Now all of the terms in this equation are energies. When γ > 1, we have non-zero kinetic energy. So, if we think of γmc2 as the total energy of body, and write
then (γ - 1)*mc2 is the kinetic energy, and 1*mc2 is an energy that a body has when v = 0 and γ = 1.

Remember the proper time and proper length of module 4. These were the time and length of a body measured in its own frame. So we could write

where E0 = mc2 is the proper energy of a body - the energy that it has, even when it is not moving. So that famous equation, E0 = mc2, has come from identification of the constant of integration in the relativistic version of the work-energy theorem.
    Given that it's such an important equation, it's interesting to ask: Is this identification of the proper energy a derivation or an inspired guess on Einstein's part? My judgment would be somewhere between the two.
We are getting used to large numbers, but let's remember that
    c2 = 9.0 x 1016 m2s-2 = 9.0 x 1016 J/kg.
Yes, c2 has units of joules per kilogram, as we can see from the familiar expression Kclassical = ½mv2. So the conversion of one kilogram mass would liberate nearly 1017 joules. Ouch! (By the way, this is not a feature restricted to nuclear energy: See the discussion of binding energy, and the example below.)

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