The Open Door Web Site
Relativity

Relativistic Mass

Consider the situation shown below.

A and B are initially at relative rest. B then accelerates away from A using a constant force.

After time t (as measured by B), B meets C and for a short time B stops the rocket motor so as to move with zero velocity relative to C.

During this short time, A measures the velocity of B (and C), and finds it to be 05c.


B now restarts the rocket motor. After time t (measured by B, as before) the situation as observed by C must be as shown below.

Now, let us transform Cs observations to As reference frame.

Velocity of B relative to A is v.

Therefore, during the first period of acceleration, the velocity of B relative to A changed by 05c. During the second period of acceleration, it only changed by 03c but we have stated that the force causing the acceleration was constant.

We must conclude that from As point of view, the inertia of B steadily increased.

Conclusion

The mass of a body is a relative concept.

The mass of a body measured by an observer at rest relative to the body is called (not surprisingly) the rest mass of the body.

The mass (sometimes called the relativistic mass) of the body measured by other observers depends on the velocity of the observer relative to the body.

As the variation of mass is basically due to the time dilation effect, you should not be surprised to find that, if the rest mass of a body is mo, then its mass, m, as measured by an observer moving with speed v relative to the body is given by

m = mo/(1 v2/c2)

Relativistic Momentum

As in Newtonian mechanics, the momentum of a body is often useful in the solution of problems. Momentum is the product of mass and velocity so, relativistic momentum is given by

p = vmo/(1 v2/c2)

In other words, relativistic momentum is calculated by simply taking the Newtonian definition of momentum but remembering that mass is now a variable quantity.

This can not be done with the kinetic energy of a body.

Mass and Energy

If a force causes body B to accelerate away from observer A (as in the example above) then work is done by that force. As usual we can define the kinetic energy possessed by body B (as measured by A) by saying that

K.E. of B = Work Done causing it to accelerate

It can be shown that if the relative speed of body B is such that its mass (as measured by A) is m, then

K.E. = mc2 - moc2 or K.E. = (change in mass)c2

Here we are seeing the equivalence of mass and energy. Some of the work done by the force is converted into mass and if we define the total energy, E, possessed by a body to be the sum of its rest energy (moc2) and its K.E. we have the famous result

DELTA01E = DELTA01mc2

 

It is easy to show that if the velocity of the body relative to the observer is small compared with the velocity of light, then the relativistic formula reduces to the Newtonian expression (mv2)

If the velocity of the body relative to the observer is very close to the velocity of light, virtually all the work done by the force is converted to mass.

Experiments involving high speed particles (protons, electrons etc.) in particle accelerators give evidence to support the idea that mass varies with velocity.

Units of Mass/Energy

The S.I. unit for mass is the kg and for energy, the Joule. However, on the scale of subatomic particles, we often use MeV for energy (1MeV = 1610-13J). So, a possible unit for the quantity "mc2" is MeV.

For this reason, the masses of subatomic particles are often expressed in MeV/c2.

For example the rest energy of an electron is about 511MeV and its mass is therefore said to be 511MeV/c2.


 

Privacy Policy

Copyright Information

Sponsored Links

Sponsored Pages

Donating to the ODWS

Advertising on the ODWS