# 5.8 Relativistic momentum

 Page 1 / 3
By the end of this section, you will be able to:
• Define relativistic momentum in terms of mass and velocity
• Show how relativistic momentum relates to classical momentum
• Show how conservation of relativistic momentum limits objects with mass to speeds less than $c$

Momentum is a central concept in physics. The broadest form of Newton’s second law is stated in terms of momentum. Momentum is conserved whenever the net external force on a system is zero. This makes momentum conservation a fundamental tool for analyzing collisions ( [link] ). Much of what we know about subatomic structure comes from the analysis of collisions of accelerator-produced relativistic particles, and momentum conservation plays a crucial role in this analysis.

The first postulate of relativity states that the laws of physics are the same in all inertial frames. Does the law of conservation of momentum survive this requirement at high velocities? It can be shown that the momentum calculated as merely $\stackrel{\to }{p}=m\frac{d\stackrel{\to }{x}}{dt},$ even if it is conserved in one frame of reference, may not be conserved in another after applying the Lorentz transformation to the velocities. The correct equation for momentum can be shown, instead, to be the classical expression in terms of the increment $d\tau$ of proper time of the particle, observed in the particle’s rest frame:

$\begin{array}{cc}\hfill \stackrel{\to }{p}& =m\frac{d\stackrel{\to }{x}}{d\tau }=m\frac{d\stackrel{\to }{x}}{dt}\phantom{\rule{0.1em}{0ex}}\frac{dt}{d\tau }\hfill \\ & =m\frac{d\stackrel{\to }{x}}{dt}\phantom{\rule{0.2em}{0ex}}\frac{1}{\sqrt{1-{u}^{2}\text{/}{c}^{2}}}\hfill \\ & =\frac{m\stackrel{\to }{u}}{\sqrt{1-{u}^{2}\text{/}{c}^{2}}}=\gamma m\stackrel{\to }{u}.\hfill \end{array}$

## Relativistic momentum

Relativistic momentum $\stackrel{\to }{p}$ is classical momentum multiplied by the relativistic factor γ :

$\stackrel{\to }{p}=\gamma m\stackrel{\to }{u}$

where m is the rest mass    of the object, $\stackrel{\to }{u}$ is its velocity relative to an observer, and γ is the relativistic factor:

$\gamma =\frac{1}{\sqrt{1-\frac{{u}^{2}}{{c}^{2}}}}.$

Note that we use u for velocity here to distinguish it from relative velocity v between observers. The factor $\gamma$ that occurs here has the same form as the previous relativistic factor $\gamma$ except that it is now in terms of the velocity of the particle u instead of the relative velocity v of two frames of reference.

With p expressed in this way, total momentum ${p}_{\text{tot}}$ is conserved whenever the net external force is zero, just as in classical physics. Again we see that the relativistic quantity becomes virtually the same as the classical quantity at low velocities, where u / c is small and $\gamma$ is very nearly equal to 1. Relativistic momentum has the same intuitive role as classical momentum. It is greatest for large masses moving at high velocities, but because of the factor $\gamma ,$ relativistic momentum approaches infinity as u approaches c ( [link] ). This is another indication that an object with mass cannot reach the speed of light. If it did, its momentum would become infinite—an unreasonable value.

The relativistically correct definition of momentum as $p=\gamma mu$ is sometimes taken to imply that mass varies with velocity: ${m}_{\text{var}}=\gamma m,$ particularly in older textbooks. However, note that m is the mass of the object as measured by a person at rest relative to the object. Thus, m is defined to be the rest mass, which could be measured at rest, perhaps using gravity. When a mass is moving relative to an observer, the only way that its mass can be determined is through collisions or other means involving momentum. Because the mass of a moving object cannot be determined independently of momentum, the only meaningful mass is rest mass. Therefore, when we use the term “mass,” assume it to be identical to “rest mass.”

Relativistic momentum is defined in such a way that conservation of momentum holds in all inertial frames. Whenever the net external force on a system is zero, relativistic momentum is conserved, just as is the case for classical momentum. This has been verified in numerous experiments.

Check Your Understanding What is the momentum of an electron traveling at a speed 0.985 c ? The rest mass of the electron is $9.11\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-31}\text{kg}.$

Substitute the data into the given equation:
$p=\gamma mu=\frac{mu}{\sqrt{1-\frac{{u}^{2}}{{c}^{2}}}}=\frac{\left(9.11\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-31}\phantom{\rule{0.2em}{0ex}}\text{kg}\right)\left(0.985\right)\left(3.00\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{8}\phantom{\rule{0.2em}{0ex}}\text{m/s}\right)}{\sqrt{1-\frac{{\left(0.985c\right)}^{2}}{{c}^{2}}}}=1.56\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-21}\phantom{\rule{0.2em}{0ex}}\text{kg-m/s.}$

## Summary

• The law of conservation of momentum is valid for relativistic momentum whenever the net external force is zero. The relativistic momentum is $p=\gamma mu,$ where m is the rest mass of the object, u is its velocity relative to an observer, and the relativistic factor is $\gamma =\frac{1}{\sqrt{1-\frac{{u}^{2}}{{c}^{2}}}}.$
• At low velocities, relativistic momentum is equivalent to classical momentum.
• Relativistic momentum approaches infinity as u approaches c . This implies that an object with mass cannot reach the speed of light.

## Conceptual questions

How does modern relativity modify the law of conservation of momentum?

Is it possible for an external force to be acting on a system and relativistic momentum to be conserved? Explain.

Yes. This can happen if the external force is balanced by other externally applied forces, so that the net external force is zero.

## Problems

Find the momentum of a helium nucleus having a mass of $6.68\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-27}\phantom{\rule{0.2em}{0ex}}\text{kg}$ that is moving at 0.200 c .

$4.09\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-19}\phantom{\rule{0.2em}{0ex}}\text{kg}·\text{m/s}$

What is the momentum of an electron traveling at 0.980 c ?

(a) Find the momentum of a $1.00\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{9}\text{-kg}$ asteroid heading towards Earth at 30.0 km/s. (b) Find the ratio of this momentum to the classical momentum. (Hint: Use the approximation that $\gamma =1+\left(1\text{/}2\right){v}^{2}\text{/}{c}^{2}$ at low velocities.)

a. $3.000000015\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{13}\phantom{\rule{0.2em}{0ex}}\text{kg}·\text{m/s;}$ b. 1.000000005

(a) What is the momentum of a 2000-kg satellite orbiting at 4.00 km/s? (b) Find the ratio of this momentum to the classical momentum. (Hint: Use the approximation that $\gamma =1+\left(1\text{/}2\right){v}^{2}\text{/}{c}^{2}$ at low velocities.)

What is the velocity of an electron that has a momentum of $3.04\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-21}\phantom{\rule{0.2em}{0ex}}\text{kg}·\text{m/s}$ ? Note that you must calculate the velocity to at least four digits to see the difference from c .

$2.988\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{8}\phantom{\rule{0.2em}{0ex}}\text{m/s}$

Find the velocity of a proton that has a momentum of $4.48\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{-19}\phantom{\rule{0.2em}{0ex}}\text{kg}·\text{m/s}\text{.}$

in the wave equation y=Asin(kx-wt+¢) what does k and w stand for.
k is the wave number and w rotational speed
Mwezi
derivation of lateral shieft
Hi
Hi
hi
ALFRED
how are you?
hi
asif
hi
Imran
I'm fine
ALFRED
total binding energy of ionic crystal at equilibrium is
How does, ray of light coming form focus, behaves in concave mirror after refraction?
Sushant
What is motion
Anything which changes itself with respect to time or surrounding
Sushant
good
Chemist
and what's time? is time everywhere same
Chemist
No
Sushant
how can u say that
Chemist
do u know about black hole
Chemist
Not so more
Sushant
DHEERAJ
Sushant
But ask anything changes itself with respect to time or surrounding A Not any harmful radiation
DHEERAJ
explain cavendish experiment to determine the value of gravitational concept.
For the question about the scuba instructor's head above the pool, how did you arrive at this answer? What is the process?
as a free falling object increases speed what is happening to the acceleration
of course g is constant
Alwielland
acceleration also inc
Usman
which paper will be subjective and which one objective
jay
normal distributiin of errors report
Dennis
normal distribution of errors
Dennis
photo electrons doesn't emmit when electrons are free to move on surface of metal why?
What would be the minimum work function of a metal have to be for visible light(400-700)nm to ejected photoelectrons?
give any fix value to wave length
Rafi
40 cm into change mm
40cm=40.0×10^-2m =400.0×10^-3m =400mm. that cap(^) I have used above is to the power.
Prema
i.e. 10to the power -2 in the first line and 10 to the power -3 in the the second line.
Prema
there is mistake in my first msg correction is 40cm=40.0×10^-2m =400.0×10^-3m =400mm. sorry for the mistake friends.
Prema
40cm=40.0×10^-2m =400.0×10^-3m =400mm.
Prema
this msg is out of mistake. sorry friends​.
Prema
what is physics?
why we have physics
because is the study of mater and natural world
John
because physics is nature. it explains the laws of nature. some laws already discovered. some laws yet to be discovered.
Yoblaze
physics is the study of non living things if we added it with biology it becomes biophysics and bio is the study of living things tell me please what is this?
tahreem
physics is the study of matter,energy and their interactions
Buvanes
all living things are matter
Buvanes
why rolling friction is less than sliding friction
tahreem
thanks buvanas
tahreem
is this a physics forum
explain l-s coupling