Contents

Relativistic Addition of Velocities

A man with oar in his hand is kayaking downstream in a shallow fast-flowing river.

Figure 28.13 The total velocity of a kayak, like this one on the Deerfield River in Massachusetts, is its velocity relative to the water as well as the water’s velocity relative to the riverbank. (credit: abkfenris, Flickr)

If you’ve ever seen a kayak move down a fast-moving river, you know that remaining in the same place would be hard. The river current pulls the kayak along. Pushing the oars back against the water can move the kayak forward in the water, but that only accounts for part of the velocity. The kayak’s motion is an example of classical addition of velocities. In classical physics, velocities add as vectors. The kayak’s velocity is the vector sum of its velocity relative to the water and the water’s velocity relative to the riverbank.

Classical Velocity Addition

For simplicity, we restrict our consideration of velocity addition to one-dimensional motion. Classically, velocities add like regular numbers in one-dimensional motion. (See Figure 28.14.) Suppose, for example, a girl is riding in a sled at a speed 1.0 m/s relative to an observer. She throws a snowball first forward, then backward at a speed of 1.5 m/s relative to the sled. We denote direction with plus and minus signs in one dimension; in this example, forward is positive. Let $v v size 12{v} {}$ be the velocity of the sled relative to the Earth, $u u size 12{u} {}$ the velocity of the snowball relative to the Earth-bound observer, and $u' u' size 12{u rSup { size 8{'} } } {}$ the velocity of the snowball relative to the sled.

In part a, a man is pulling a sled towards the right with a velocity v equals one point zero meters per second. A girl sitting on the sled facing forward throws a snowball toward a boy on the far right of the picture. The snowball is labeled u primed equals one point five meters per second in the direction the sled is being pulled. The boy is labelled two point five meters per second. In figure b, a similar figure is shown, but the man’s velocity is one point zero meters per second, the girl is facing backward and throwing the snowball behind the sled. The snowball is labelled u primed equals negative one point five meters per second, and the boy is labelled u equals negative zero point five meters per second.

Figure 28.14 Classically, velocities add like ordinary numbers in one-dimensional motion. Here the girl throws a snowball forward and then backward from a sled. The velocity of the sled relative to the Earth is

v= 1.0 m/s v= 1.0 size 12{ ital "v="1 "." 0`"m/s"} {}

. The velocity of the snowball relative to the sled is

u' u' size 12{u rSup { size 8{'} } } {}

, while its velocity relative to the Earth is

u u size 12{u} {}

. Classically,

u=v+u' u=v+u'

Classical Velocity Addition

u=v+u' u=v+u'

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Thus, when the girl throws the snowball forward, $u = 1.0 m/s + 1.5 m/s = 2.5 m/s u = 1.0 m/s + 1.5 m/s = 2.5 m/s$ . It makes good intuitive sense that the snowball will head towards the Earth-bound observer faster, because it is thrown forward from a moving vehicle. When the girl throws the snowball backward, $u = 1.0 m/s + (- 1.5 m/s) = - 0.5 m/s u = 1.0 m/s + (- 1.5 m/s) = - 0.5 m/s$ . The minus sign means the snowball moves away from the Earth-bound observer.

Relativistic Velocity Addition

The second postulate of relativity (verified by extensive experimental observation) says that classical velocity addition does not apply to light. Imagine a car traveling at night along a straight road, as in Figure 28.15. If classical velocity addition applied to light, then the light from the car’s headlights would approach the observer on the sidewalk at a speed $u=v+c u=v+c size 12{ ital "u=v+c"} {}$ . But we know that light will move away from the car at speed $c c size 12{c} {}$ relative to the driver of the car, and light will move towards the observer on the sidewalk at speed $c c size 12{c} {}$ , too.

A car is moving towards right with velocity v. A boy standing on the side-walk observes the car. The velocity of light u primed is shown to be c as observed by the girl in the car and the velocity of light u is also c as observed by the boy.

Figure 28.15 According to experiment and the second postulate of relativity, light from the car’s headlights moves away from the car at speed

c c size 12{c} {}

and towards the observer on the sidewalk at speed

c c size 12{c} {}

. Classical velocity addition is not valid.

Relativistic Velocity Addition

Either light is an exception, or the classical velocity addition formula only works at low velocities. The latter is the case. The correct formula for one-dimensional relativistic velocity addition is

u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}}, u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}}, size 12{ ital "u=" {  { ital "v+u'"}  over  {1+ {  {v` ital "u'"}  over  {c rSup { size 8{2} } } } } } } {}

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where $v v$ is the relative velocity between two observers, $u u$ is the velocity of an object relative to one observer, and $u' u'$ is the velocity relative to the other observer. (For ease of visualization, we often choose to measure $u u$ in our reference frame, while someone moving at $v v$ relative to us measures $u' u'$ .) Note that the term $\frac{v u'}{c^{2}} \frac{v u'}{c^{2}}$ becomes very small at low velocities, and $u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}} u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}}$ gives a result very close to classical velocity addition. As before, we see that classical velocity addition is an excellent approximation to the correct relativistic formula for small velocities. No wonder that it seems correct in our experience.

Example 28.3

Showing that the Speed of Light towards an Observer is Constant (in a Vacuum): The Speed of Light is the Speed of Light

Suppose a spaceship heading directly towards the Earth at half the speed of light sends a signal to us on a laser-produced beam of light. Given that the light leaves the ship at speed $c c size 12{c} {}$ as observed from the ship, calculate the speed at which it approaches the Earth.

A spacecraft is heading towards earth v equals zero point five zero zero times c. A laser beam from the ship travels towards the Earth with velocity c as shown by a vector. A second spaceship traveling away from the Earth. The velocity of the second ship and second laser are the same as the first, but in the opposite direction.

Figure 28.16

Strategy

Because the light and the spaceship are moving at relativistic speeds, we cannot use simple velocity addition. Instead, we can determine the speed at which the light approaches the Earth using relativistic velocity addition.

Solution

Identify the knowns. $v= 0.500 c v= 0.500 c$ ; $u' = c u' = c$
Identify the unknown. $u u size 12{u} {}$
Choose the appropriate equation. $u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}} u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}} size 12{ ital "u=" { { ital "v+u'"} over {1+ { {v` ital "u'"} over {c rSup { size 8{2} } } } } } } {}$
Plug the knowns into the equation.
$\begin{array}{l} u & = & \frac{v+u'}{1 + \frac{v u'}{c^{2}}} \\ = & \frac{0.500 c + c}{1 + \frac{(0.500 c) (c)}{c^{2}}} \\ = & \frac{(0.500 + 1) c}{1 + \frac{0.500 c^{2}}{c^{2}}} \\ = & \frac{1.500 c}{1 + 0.500} \\ = & \frac{1.500 c}{1.500} \\ = & c \end{array} \begin{array}{l} u & = & \frac{v+u'}{1 + \frac{v u'}{c^{2}}} \\ = \frac{0.500 c + c}{1 + \frac{(0.500 c) (c)}{c^{2}}} \\ = \frac{(0.500 + 1) c}{1 + \frac{0.500 c^{2}}{c^{2}}} \\ = \frac{1.500 c}{1 + 0.500} \\ = \frac{1.500 c}{1.500} \\ = c \end{array}$
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Discussion

Relativistic velocity addition gives the correct result. Light leaves the ship at speed $c c size 12{c} {}$ and approaches the Earth at speed $c c size 12{c} {}$ . The speed of light is independent of the relative motion of source and observer, whether the observer is on the ship or Earth-bound.

Velocities cannot add to greater than the speed of light, provided that $v v size 12{v} {}$ is less than $c c size 12{c} {}$ and $u' u'$ does not exceed $c c$ . The following example illustrates that relativistic velocity addition is not as symmetric as classical velocity addition.

Example 28.4

Comparing the Speed of Light towards and away from an Observer: Relativistic Package Delivery

Suppose the spaceship in the previous example is approaching the Earth at half the speed of light and shoots a canister at a speed of $0.750 c 0.750 c$ . (a) At what velocity will an Earth-bound observer see the canister if it is shot directly towards the Earth? (b) If it is shot directly away from the Earth? (See Figure 28.17.)

In part a, a spaceship is moving towards the earth from left to right with a velocity v equals to zero point five zero times c. The spaceships shoots a canister towards earth with velocity u prime equals zero point seven five times c. A man stands stationary on earth observing. In part b, the spaceship shoots the canister away from earth with same velocity. In both the cases, the velocity of the ship is v equals 0 point five zero times c toward left.

Figure 28.17

Strategy

Because the canister and the spaceship are moving at relativistic speeds, we must determine the speed of the canister by an Earth-bound observer using relativistic velocity addition instead of simple velocity addition.

Solution for (a)

Identify the knowns. $v= 0.500 c v= 0.500 c$ ; $u' = 0 . 750 c u' = 0 . 750 c size 12{u rSup { size 8{'} } = - 0 "." "750"c} {}$
Identify the unknown. $u u size 12{u} {}$
Choose the appropriate equation. $u= \frac{v+u'}{1 + \frac{v u'}{c^{2}}} u= \frac{v+u'}{1 + \frac{v u'}{c^{2}}}$
Plug the knowns into the equation.
$\begin{array}{l} u & = & \frac{v+u'}{1 + \frac{v u'}{c^{2}}} \\ = & \frac{0.500 c + 0.750 c}{1 + \frac{(0.500 c) (0.750 c)}{c^{2}}} \\ = & \frac{1.250 c}{1 + 0.375} \\ = & 0.909 c \end{array} \begin{array}{l} u & = & \frac{v+u'}{1 + \frac{v u'}{c^{2}}} \\ = \frac{0.500 c + 0.750 c}{1 + \frac{(0.500 c) (0.750 c)}{c^{2}}} \\ = \frac{1.250 c}{1 + 0.375} \\ = 0.909 c \end{array}$
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Solution for (b)

Identify the knowns. $v = 0.500 c v = 0.500 c$ ; $u' = - 0.750 c u' = - 0.750 c$
Identify the unknown. $u u$
Choose the appropriate equation. $u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}} u = \frac{v+u'}{1 + \frac{v u'}{c^{2}}}$
Plug the knowns into the equation.
$\begin{array}{l} u & = & \frac{v+u'}{1 + \frac{v u'}{c^{2}}} \\ = & \frac{0.500 c + (- 0.750 c)}{1 + \frac{(0.500 c) (- 0.750 c)}{c^{2}}} \\ = & \frac{- 0.250 c}{1 - 0.375} \\ = & - 0.400 c \end{array} \begin{array}{l} u & = & \frac{v+u'}{1 + \frac{v u'}{c^{2}}} \\ = \frac{0.500 c + (- 0.750 c)}{1 + \frac{(0.500 c) (- 0.750 c)}{c^{2}}} \\ = \frac{- 0.250 c}{1 - 0.375} \\ = - 0.400 c \end{array}$
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Discussion

The minus sign indicates velocity away from the Earth (in the opposite direction from $v v$ ), which means the canister is heading towards the Earth in part (a) and away in part (b), as expected. But relativistic velocities do not add as simply as they do classically. In part (a), the canister does approach the Earth faster, but not at the simple sum of $1.250 c 1.250 c$ . The total velocity is less than you would get classically. And in part (b), the canister moves away from the Earth at a velocity of $- 0.400 c - 0.400 c$ , which is faster than the $−0.250 c −0.250 c size 12{c} {}$ you would expect classically. The velocities are not even symmetric. In part (a) the canister moves $0.409 c 0.409 c size 12{c} {}$ faster than the ship relative to the Earth, whereas in part (b) it moves $0.900 c 0.900 c size 12{c} {}$ slower than the ship.

Doppler Shift

Although the speed of light does not change with relative velocity, the frequencies and wavelengths of light do. First discussed for sound waves, a Doppler shift occurs in any wave when there is relative motion between source and observer.

Relativistic Doppler Effects

The observed wavelength of electromagnetic radiation is longer (called a red shift) than that emitted by the source when the source moves away from the observer and shorter (called a blue shift) when the source moves towards the observer.

{=λ}_{obs} {=λ}_{s} \sqrt{\frac{1 + \frac{u}{c}}{1 - \frac{u}{c}}} . {=λ}_{obs} {=λ}_{s} \sqrt{\frac{1 + \frac{u}{c}}{1 - \frac{u}{c}}} . size 12{λ rSub { size 8{"obs"} }  ital "=λ" rSub { size 8{s} }  sqrt { {  {1+ {  {u}  over  {c} } }  over  {1 -  {  {u}  over  {c} } } } } } {}

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In the Doppler equation, $λ_{obs} λ_{obs} size 12{λ rSub { size 8{"obs"} } } {}$ is the observed wavelength, $λ_{s} λ_{s} size 12{λ rSub { size 8{s} } } {}$ is the source wavelength, and $u u size 12{u} {}$ is the relative velocity of the source to the observer. The velocity $u u size 12{u} {}$ is positive for motion away from an observer and negative for motion toward an observer. In terms of source frequency and observed frequency, this equation can be written

f_{obs} {=f}_{s} \sqrt{\frac{1 - \frac{u}{c}}{1 + \frac{u}{c}}} . f_{obs} {=f}_{s} \sqrt{\frac{1 - \frac{u}{c}}{1 + \frac{u}{c}}} . size 12{f rSub { size 8{"obs"} }  ital "=f" rSub { size 8{s} }  sqrt { {  {1 -  {  {u}  over  {c} } }  over  {1+ {  {u}  over  {c} } } } } } {}

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Notice that the – and + signs are different than in the wavelength equation.

Career Connection: Astronomer

If you are interested in a career that requires a knowledge of special relativity, there’s probably no better connection than astronomy. Astronomers must take into account relativistic effects when they calculate distances, times, and speeds of black holes, galaxies, quasars, and all other astronomical objects. To have a career in astronomy, you need at least an undergraduate degree in either physics or astronomy, but a Master’s or doctoral degree is often required. You also need a good background in high-level mathematics.

Example 28.5

Calculating a Doppler Shift: Radio Waves from a Receding Galaxy

Suppose a galaxy is moving away from the Earth at a speed $0.825 c 0.825 c$ . It emits radio waves with a wavelength of $0.525 m 0.525 size 12{0 "." "525"" m"} {}$ . What wavelength would we detect on the Earth?

Strategy

Because the galaxy is moving at a relativistic speed, we must determine the Doppler shift of the radio waves using the relativistic Doppler shift instead of the classical Doppler shift.

Solution

Identify the knowns. $u= 0.825 c u= 0.825 c size 12{ ital "u="0 "." "825"c} {}$ ; $λ_{s} = 0 . 525 m λ_{s} = 0 . 525 size 12{λ rSub { size 8{s} } =0 "." "525"`m} {}$
Identify the unknown. $λ_{obs} λ_{obs} size 12{λ rSub { size 8{"obs"} } } {}$
Choose the appropriate equation. $λ_{obs} {=λ}_{s} \sqrt{\frac{1 + \frac{u}{c}}{1 - \frac{u}{c}}} λ_{obs} {=λ}_{s} \sqrt{\frac{1 + \frac{u}{c}}{1 - \frac{u}{c}}} size 12{λ rSub { size 8{"obs"} } ital "=λ" rSub { size 8{s} } sqrt { { {1+ { {u} over {c} } } over {1 - { {u} over {c} } } } } } {}$
Plug the knowns into the equation.
$\begin{array}{l} λ_{obs} & = & λ_{s} \sqrt{\frac{1 + \frac{u}{c}}{1 - \frac{u}{c}}} \\ = & (0.525 m) \sqrt{\frac{1 + \frac{0.825 c}{c}}{1 - \frac{0.825 c}{c}}} \\ = & 1.70 m. \end{array} \begin{array}{l} λ_{obs} & = & λ_{s} \sqrt{\frac{1 + \frac{u}{c}}{1 - \frac{u}{c}}} \\ = (0.525 m) \sqrt{\frac{1 + \frac{0.825 c}{c}}{1 - \frac{0.825 c}{c}}} \\ = 1.70 m. \end{array}$
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Discussion

Because the galaxy is moving away from the Earth, we expect the wavelengths of radiation it emits to be redshifted. The wavelength we calculated is 1.70 m, which is redshifted from the original wavelength of 0.525 m.

The relativistic Doppler shift is easy to observe. This equation has everyday applications ranging from Doppler-shifted radar velocity measurements of transportation to Doppler-radar storm monitoring. In astronomical observations, the relativistic Doppler shift provides velocity information such as the motion and distance of stars.

Check Your Understanding

Suppose a space probe moves away from the Earth at a speed $0.350 c 0.350 c size 12{0 "." "350"c} {}$ . It sends a radio wave message back to the Earth at a frequency of 1.50 GHz. At what frequency is the message received on the Earth?

Show solution

Solution

f_{obs} {=f}_{s} \sqrt{\frac{1 - \frac{u}{c}}{1 + \frac{u}{c}}} = (1 . 50 GHz) \sqrt{\frac{1 - \frac{0.350 c}{c}}{1 + \frac{0.350 c}{c}}} = 1 . 04 GHz f_{obs} {=f}_{s} \sqrt{\frac{1 - \frac{u}{c}}{1 + \frac{u}{c}}} = (1 . 50 GHz) \sqrt{\frac{1 - \frac{0.350 c}{c}}{1 + \frac{0.350 c}{c}}} = 1 . 04 GHz size 12{f rSub { size 8{"obs"} }  ital "=f" rSub { size 8{s} }  sqrt { {  {1 -  {  {u}  over  {c} } }  over  {1+ {  {u}  over  {c} } } } } = \( 1 "." "50 GHz" \)  sqrt { {  {1 -  {  {0 "." "350" ital " c"}  over  {c} } }  over  {1+ {  {0 "." "350" ital " c"}  over  {c} } } } } =1 "." "04 GHz"} {}

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