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While looking at some exercises in my physics textbook, I came across the following problem which I thought was quite interesting:

It is possible for the electron beam in a television picture tube to move across the screen at a speed faster than the speed of light.

Why does this not contradict special relativity?

I suspect that it's because the television is in air, and light in air travels slower than light in a vacuum. So I suppose they're saying the the electron could travel faster in air than the speed of light in air, like what causes Cherenkov radiation?

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    $\begingroup$ You could also just consider a person shining a laser pointer at a distant wall. As you spin around, the spot of the laser pointer moves on the wall with a speed dependent on the distance to the wall. In principle, the wall could be so far away that the spot moves faster than the speed of light. But the light is still moving at the speed of light (in air, or whatever). The spot is not really an object - unless you are the inmate trying to escape from the insane asylum on a beam of light! $\endgroup$
    – Greg P
    Commented Dec 28, 2010 at 22:17
  • $\begingroup$ @Greg oh! move across the screen... so is it talking about the picture itself? I thought it was saying the beam from the electron gun was moving faster than light $\endgroup$ Commented Dec 28, 2010 at 22:21
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    $\begingroup$ Yes. It is something I remember from an intro relativity book. It means the actual spot (yes, the image) moving across the screen. Otherwise, I don't get the point of the question. The electrons themselves don't move faster than light. It is just an illusion of something moving faster than the speed of light. $\endgroup$
    – Greg P
    Commented Dec 28, 2010 at 22:31
  • $\begingroup$ There were some other 'paradoxes' where objects seem to move at superluminal speeds. Particularly one from astrophysics which seemed interesting...perhaps someone can remember it for me. $\endgroup$
    – Greg P
    Commented Dec 28, 2010 at 22:35
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    $\begingroup$ @GregP: en.wikipedia.org/wiki/Superluminal_motion has some descriptions of common examples. Although that might be a good question to ask on the site. $\endgroup$
    – David Z
    Commented Dec 28, 2010 at 23:47

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This is an example of what is sometimes called the "Marquee Effect." Think of the light bulbs surrounding an old-fashioned movie theater marquee, where the light bulbs turn on in sequence to produce the illusion, from a distance, of a light source which is moving around the the marquee.

There is no limit on how short the time interval is between one light turning on and the next turning on, so the perceived light source position can move arbitrarily fast, but in fact nothing is actually moving at all.

In the case of the television screen, the phosphors on the screen can be lit in rapid sequence, but the electrons in the beam do not ever need to move at (or even near) the speed of light.

More generally, there are loads of examples of some imaginary or conceptual "object" moving faster than light, but in all these cases there is nothing actually moving at all. A classic example is the intersection point of two nearly parallel lines, which moves very rapidly as the angle between the lines changes. In this case it is obvious that the moving "object" isn't moving at all, but its still a good example of a case where you can discuss something moving faster than light without there being any violation of physical law.

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This is a conflation of phase velocity, and group velocity. The beam can be seen to move from say left to right at higher than c, but no information or particles are traveling that fast. Information is being transmitted from the electron gun to the phosphor at well under the speed of light.

It has nothing to do with the media it is embedded in. The information is going from the electron gun to the screen, not from one location on the screen to another.

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  • $\begingroup$ How come the beam is a wave? $\endgroup$ Commented Dec 28, 2010 at 22:12
  • $\begingroup$ @wrongusername: A beam of electrons behaves like a wave beam, the same is behaviour is verified even in much larger particles (such as small atoms). The reason lies in Quantum Mechanics, and I can't get into it here. $\endgroup$
    – Malabarba
    Commented Dec 28, 2010 at 22:47
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    $\begingroup$ All of this is mostly irrelevant though, as the wave nature of the beam has nothing to do with your question. This could happen with virtually anything that moves. $\endgroup$
    – Malabarba
    Commented Dec 28, 2010 at 22:48
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    $\begingroup$ Replace the electron beam with a marshmallow gun. People think of quantum theory and waves when they hear "electron" but not with "marshmallows". Of course, it may be hard to actually create a series of marshmallow collisions on a distant wall appearing to move faster than c, but heck this is only a thought experiment, so imagine if you have a powerful enough gun... $\endgroup$
    – DarenW
    Commented Mar 5, 2011 at 21:17
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There is no contradiction in "processes" made up of sequences of independent events such as these because there is no causal relationship between the individual events - in this case the flights of the individual electrons and their ultimate collision with the screen - that make up the process.

If the screen is far enough from the source and the scan so fast then the sequence of electron collisions moves across the screen at faster than $c$. In this case, the order of the collisions on the screen is reversed when observed from an inertial frame moving fast enough against the direction of motion of the scan. This is simply a manifestation of relativity of simultaneity. But this is not a problem, because each of the electron flights is causally independent, and therefore there is no possibility of a violation of causality wrought by the frame's motion.

It is, however, a problem if the sub-events making up the process are causally related. This would be so if the motion were that of lone electron, where its being ($B$) at each instant is causally related to its being at any former instant ($A$) - $A$ is then a cause of $B$. One can then find a relatively moving frame, for example, where each electron would fly back into the cathode, undergo inverse thermionic emission and become a conduction electron again.

Indeed the above is the primary reason why we postulate that such faster than light motion is forbidden in relativity: it would violate causality and we make this postulate to uphold a causal description of the universe.

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Here's another example from Griffith's book "Introduction to Electrodynamics" which illustrates phenomena where what we see is not what we observe. The apparent speed can be much greater than the speed of light. This speed is just what we see, an illusion, and it's the result of our inability sometimes to see the actual direction of movement of an distant object w.r.t. us and the fact that the light needs some finite time to get to our eyes.

Problem 12.6 Every 2 years, more or less, The New York Times publishes

an article in which some astronomer claims to have found an object

traveling faster than the speed of light. Many of these reports

result from a failure to distinguish what is seen from what is

observed--that is, from a failure to account for light travel time.

Here's an example: A star is traveling with speed $v$ at an angle $\theta$ to

the line of sight (Fig. 12.6). What is its apparent speed across the

sky'?

enter image description here

(Suppose the light signal from $b$ reaches the earth at a time At after

the signal from a, and the star has meanwhile advanced a distance $\Delta s$

across the celestial sphere; by "apparent speed" I mean $\Delta s/\Delta t$.) What

angle $\theta$ gives the maximum apparent speed? Show that the apparent

speed can be much greater than $c$, even if $v$ itself is less than $c$.

It can be easily shown that the apparent speed in this example is:

$u_{app}=\frac{v\sin\theta}{1-\frac{v}{c}\cos\theta}$

To find the angle $\theta$ that gives the maximum apparent speed we just differentiate and solve, for $\theta$, the equation:

$\frac{d u_{app}}{d\theta}=0 \Leftrightarrow \theta_{max}=\cos^{-1}(\frac{v}{c})$

At this angle, $u_{app}=\frac{v}{\sqrt{1-v^2/c^2}}=\gamma v$

This result shows that when $v\to c$, $u_{app}\to \infty$, even though $v<c$.

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    $\begingroup$ This is not quite the same issue as in the question, though. $\endgroup$
    – David Z
    Commented Jul 17, 2011 at 23:37
  • $\begingroup$ I think this is exactly the same issue. The electrons gun changes its direction, lets say by $\theta=\phi$. If we suppose that the electrons are emitted once at $\theta=0$ and once at $\theta=\phi$, we get an triangle. While the beam at $\theta=0$ travels to the screen, the electron gun rotates by $\phi$ and emits the second beam. So the time difference between the arrival of two beams can be very small. $\endgroup$
    – kuzand
    Commented Jul 17, 2011 at 23:55
  • $\begingroup$ Yes, but in the case of the electron gun (and the light bulbs, and the laser pointer, etc.), the light is being emitted by two completely different objects. Nothing actually moves even close to the speed of light. In fact, nothing has to move at all, in the case of the light bulbs. But your example with the star involves light being emitted by the same object at two separate points. Without motion, there is no superluminal effect. That's why they're different phenomena. $\endgroup$
    – David Z
    Commented Jul 18, 2011 at 0:05
  • $\begingroup$ Correction to Problem 12.6 (ought to read): "Every 2 years, more or less, The New York Time Dilations publishes an article . . ." $\endgroup$
    – Wookie
    Commented Apr 9 at 14:35
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The electron beam in a typical television moves with a speed no higher than $ 10^6 \mathrm{m/s} $, which is much less than the speed of light. I wonder what building-sized cathode ray tube television the textbook author has access to if he's made that claim.

In any case, even if the beam did move faster than the speed of light, that wouldn't cause any problem. Quoting part of the treatment of going faster than light in the Physics FAQ, section 3. Shadows and Light Spots.

Think about how fast a shadow can move. If you project the shadow of your finger using a nearby lamp onto a distant wall and then wag your finger, the shadow will move much faster than your finger. If your finger moves parallel to the wall, the shadow's speed will be multiplied by a factor $ D/d $ where $ d $ is the distance from the lamp to your finger, and $ D $ is the distance from the lamp to the wall. The speed can even be much faster than this if the wall is at an angle to your finger's motion. If the wall is very far away, the movement of the shadow will be delayed because of the time it takes light to get there, but the shadow's speed is still increased by the same ratio. The speed of a shadow is therefore not restricted to be less than the speed of light.

Others things that can go FTL include the spot of a laser that has been aimed at the surface of the Moon. Given that the distance to the Moon is 385,000 km, try working out the speed of the spot if you wave the laser at a gentle speed. You might also like to think about a water wave arriving obliquely at a long straight beach. How fast can the point at which the wave is breaking travel along the beach?

These are all examples of things that can go faster than light, but which are not physical objects. It is not possible to send information faster than light on a shadow or light spot, so FTL communication is not possible in this way. This is not what we mean by faster than light travel, although it shows how difficult it is to define what we really do mean by faster than light travel.

The electron beam in a television is very similar. The electrons are emitted from one point in the cathode ray tube, and then the direction of the beam is modified by a varying electric field. The electron beam can move from one side of the television to the other in less than $ 10^{-5} s $, but the beam doesn't carry any information from a side of the screen to the other.

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  • $\begingroup$ Re. the laser spot on the moon - suppose the laser is in a fixed position and the spot on the moon is stationary. Now I aim the laser toward a different spot on the moon arbitrarily quickly. Light has to leave the laser in the new direction and travel at speed c to get to the new target. The spot is not going to move arbitrarily quickly to the new position. So I don't get how this is an example of something (albeit non-material) moving > c. $\endgroup$ Commented Aug 19, 2020 at 0:44
  • $\begingroup$ It would indeed move arbitrarily quickly. $\endgroup$
    – Colin K
    Commented Jul 11, 2023 at 3:54
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The key idea here is a Metachronal Phenomenan, and a generalization of the Mexican Wave idea to a "Mexican Wave by Prior Arrangement".

The causal links between events in metachronal sequences can be indirect.

In particular two neigboring events in a metachoronal sequence with a spacelike separation (i.e. $c^2 \Delta t^2 - \Delta x^2 - \Delta y^2 - \Delta z^2 < 0$) can be causally "triggered" by antecedent events at arbitrary positions in their individual past light cones. Since the two light cones are not the same, the antecedent triggers can have timelike (i.e. $c^2 \Delta t^2 - \Delta x^2 - \Delta y^2 - \Delta z^2 > 0$), causal separation.

The above diagram shows two versions of a "Mexican Wave" metachronal wave disturbance, both propagating at the same, greater than $c_I$ speed: the set of events $a,\,b,\,c,\,\cdots$ and $\alpha,\,\beta,\,\gamma,\,\cdots$. The former is perfectly in keeping with causality, the latter, even though its speed is the same, is not. In the former case, a preprogrammer visits positions on the $x$ axis one after the other, leaving instructions with protagonists at these positions to make a wave movement with their arms at a mutually agreed time in the future. These acts of "preprogramming" are the events $A,\,B,\,C,\,\cdots$. The mutually agreed times arrange for the motions of each protagonist's body (the events $a,\,b,\,c,\,\cdots$) in very swift succession to one another, begetting a metachronal wave pattern that travels at greater than speed $c$ from our frame. However, there are no direct causal links $a\rightarrow b,\,b\rightarrow c,\,\cdots$, so when a relatively uniformly moving observer sees the sequence $\cdots,\,c,\,b,\,a$ reversed in their time order, there is no contradiction: all the causal links in the whole graph $\{A,\,B,\,C,\,\cdots\}\cup\{a,\,b,\,c,\,\cdots\}$ lie within the future light cone of the first event $A$ and still do so even after any Lorentz transformation effected by a relatively moving observer's motion.

Very like arguments show that the motion of a laser pointer spot across e.g. the surface of the Moon when the laser origin is on Earth, rotating in a plane at an angular speed of greater than about $45^\circ$ per second so that the spot sweeps across the Moon at greater than $300\,000{\rm km\,s^{-1}}$ is also in keeping with the principle of causality. Because the spot is moving at greater than $c$, it is seen to move in the opposite direction by some inertial observers, which fact is not a problem because there is no direct causal relationship between neighboring reflecting positions on the Moon, as for the events $a,\,b,\,c,\,\cdots$ in the diagram above. So, we can certainly see sequences of events (propagating "effects" or "things") in Nature travelling at greater than $c$, it's simply that such an observation rules out direct causal relationships between neighboring events in such a sequence.

However, as we have seen with the Wave by Prior Arrangement, such a sequence does not rule out a causal relationships between the causal forerunners or antecedents of such a sequence.

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