Can an imminent laser strike ever be observable?

  • #71
davidjoe said:
I’m not suggesting that light be slowed. And I think that is clear in the posts. Light travels at C. But objects can be accelerated to just an iota under C.
Objects can be accelerated to just under c, yes. And if you are on that object, and you measure a beam of light - any beam of light, in your object or outside it - you will measure it to be travelling at c.

davidjoe said:
If it is inconvenient that a striking difference exists in how two speeds are observed in all reference frames, when the difference between them could be the smallest possible, that doesn’t make the question or the post meaningless, does it?
What you are not factoring in is time dilation.

There is a simple scenario that involves a spaceship and a flashlight (or headlights) that shows what happens when two observers see different things, depending on where they are - I'm just not sure you're ready for it.
 
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  • #72
davidjoe said:
If it is inconvenient that a striking difference exists in how two speeds are observed in all reference frames, when the difference between them could be the smallest possible, that doesn’t make the question or the post meaningless, does it?
Yes, Special Relativity is mathematically less convenient than Galilean Relativity, but it fits observation better. Convenience is also the reason why Galilean Relativity is still being widely used, where its errors are negligible.
 
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  • #73
davidjoe said:
f the speed of light is reduced by the slightest amount
davidjoe said:
I’m not suggesting that light be slowed.
You can see why we are puzzled.
 
  • #74
Dave, I will definitely delve deeper. I have done a surface level look to see what NASA’s position is on this, just out of curiosity. Just begun so nothing to say about that.

I’m not for or against AE. I believe that is is possible to understand, be accepting of and critical of, a theory, all at the same time.

Vanadium 50 said:
You can see why we are puzzled.

Fuller context than the quote box clears that up.
 
  • #75
davidjoe said:
that doesn’t make the question or the post meaningless, does it?
It is meaningless to me. If you actually specify the precise situation and what exactly it is that the various observers are measuring then is all follows perfectly - as long as you realise that they will all see the same beam of light going past them at c. But its 'colour' may be different.
 
  • #76
sophiecentaur said:
It is meaningless to me. If you actually specify the precise situation and what exactly it is that the various observers are measuring then is all follows perfectly - as long as you realise that they will all see the same beam of light going past them at c. But its 'colour' may be different.

If it’s not striking, then it’s possible that the point blended with everything else.

Envision, we’ve left port with sister cruise line ships that are so close to our speed we never lose sight of them, right?

If I’m being overtaken in the lead at such a slow rate from the Yucatán, that only by Galveston does the sister ship pass me, … BUT should that sister ship in the rear add .0000001 MPH to it speed, I will see it go by me at light speed, well, that is striking, no?

In my hypothetical, as this turned about halfway down, everything illustrated and discussed was either my ship 2 iotas under C, a missile pursuing it 1 iota under C, or light at C, both starting a second behind me. I look at the missile for what, 100 lifetimes, but add to the missile’s speed the slightest imaginable increase in speed, which is a laser’s speed, and I would see it pass me at light speed as it if I’m completely still.
 
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  • #77
Rive said:
Nope. Light is going the fastest (straightest) between two points: anything sideways will be just slower.
In a flat space time, this is correct. In a curved space time, things are not quite so simple. There can be multiple trajectories between two events. Not all such trajectories need have equal transit times.

Consider, for instance, a laser beam that fires a few tens of meters away from your face on a starry night. It is aimed skyward at a black hole some hundreds of light years away, on a trajectory that nearly grazes the photon sphere so that the beam will loop around and come back to strike you some hundreds of years later.

In the mean time, light from dust that the beam has illuminated on its outward path might theoretically be seen hundreds of years before the final strike.
 
  • #78
davidjoe said:
I will see it go by me at light speed,
A ship cannot go at light speed. And what Lorentz Transformations give you is not what you actually see visually, but what is reconstructed to happen in a certain frame, after accounting for signal delay due to finite lightspeed.
 
  • #79
davidjoe said:
Fuller context than the quote box clears that up.
I don't think it does.

Further, we are almost 80 messages in, and we are still reading confusing and impossible things from you - despite having been shown where these are wrong. For example, "I will see it go by me at light speed" is something that material objects do not do.
 
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  • #80
Vanadium 50 said:
I don't think it does.

Further, we are almost 80 messages in, and we are still reading confusing and impossible things from you - despite having been shown where these are wrong. For example, "I will see it go by me at light speed" is something that material objects do not do.
The “it” going by me was light. And probably 4 people said that, before me. So…

If you’re referring to the cruise ships, man, is that not obviously an analogy?
 
  • #81
Apart from the illustrations, - and perhaps this is too sensitive to the core of SR to even acknowledge - but only C (a very specific speed) is claimed to be observed as constant in all reference frames.

Take away one iota from light speed, the smallest conceivable change, and now that new speed, which objects can go, is NOT observed as a constant in ALL reference frames. That new speed is frame dependent. If you are matching it, beside it, looking at it, no relative motion is perceived.

Add the small delta increase to it, which only light can go, and now you see a beam of light pass you at light speed as if you are not moving at all.
 
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  • #82
A.T. said:
A ship cannot go at light speed. And what Lorentz Transformations give you is not what you actually see visually, but what is reconstructed to happen in a certain frame, after accounting for signal delay due to finite lightspeed.

Right, a ship cannot. The three objects in question were my ship, a missile and the laser. Laser = C; missile = just under C; ship = just under laser.
 
  • #83
davidjoe said:
If you’re referring to the cruise ships, man, is that not obviously an analogy?
You can only draw valid analogies when you understand your subject. You cleasrly do not so your anaolgy means nothing.
Have you actually read around this topic or is your only inout from your questions and PF's answers? Q and A is a hopeless way of learning on-line. It actually only works well for very receptive bright minds who are 'almost there'. Your random responses have ben taking you further and further from reality because you seem not to want to be wrong.
 
  • #84
davidjoe said:
Right, a ship cannot. The three objects in question were my ship, a missile and the laser. Laser = C; missile = just under C; ship = just under laser.
No, you were talking about a "sister ship" that you "will see go by me at light speed"
davidjoe said:
should that sister ship in the rear add .0000001 MPH to it speed, I will see it go by me at light speed
As already said, a ship cannot go at light speed.
 
  • #85
A.T. said:
No, you were talking about a "sister ship" that you "will see go by me at light speed"

As already said, a ship cannot go at light speed.

Somehow the original, ship, missile, laser hypothetical image blended.

The ships were recasting the same scenario in different terms. Some of my references to the “speed of light” or maybe light speed are not to light, but to that specific speed.

I agree, completely that the final step up in speed, is made by light. But the final step up need not be a big one. That is my point.

The final step up could be an inch a year, or infinitely smaller than that. But the final step up has enormous consequences to whether all reference frames are required to see light (the speed of light in a vacuum) as a constant, or not.

That smallest change in velocity is the difference between conceivably looking at a trailing missile for millennia, (if you and it are only slightly sub C) or seeing a laser pass by you, as if you are not moving at all.
 
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  • #86
If there are only three things in the universe, your ship, the missile and the laser, from slowest to fastest, whether you are going 1 mph and the missile 2 and the laser C, or you are two iotas under C, the missile is one, and the laser passes both at C, looking at the laser, you are going to see it pass you at the difference of C.
 
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  • #87
Increasingly complicated hypotheticals will not help.
  1. There is no absolute speed. "One iota less than c" is observer dependent.
  2. Massless objects (like light) always travel at c. All observers agree on this.
  3. Massive objects always travel slower than c. Observers can disagree about their speed and even their direction.
 
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  • #88
davidjoe said:
If there are only three things in the universe, your ship, the missile and the laser, from slowest to fastest....
Some of your difficulty with relativity may come from not fully appreciating how this description is incorrect (or more precisely, includes a hidden assumption that is incorrect). It makes no sense to talk about the speed of the ship being more or less than the speed of the missile - all we can talk about is the speed of the ship relative to the missile when we consider the missile to be at rest and its negative, which will be the speed of the missile relative to the ship when we consider the ship to be at rest.
 
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  • #89
davidjoe said:
The final step up could be an inch a year, or infinitely smaller than that. But the final step up has enormous consequences to whether all reference frames are required to see light (the speed of light in a vacuum) as a constant, or not.
This is not true. The enormous consequences you speak of are due to your misunderstanding of the scenario.

It looks like you are pretending that you could get your spaceship to a tiny bit below the speed of light and everything is classical, but if you could boost it juuuuuust that little bit extra, everything would change.

No.

All things with mass, such as spaceships and atoms, move at slower than c. Always.
All massless things, such as light, move at c. Always.

You cannot swap them back and forth. You cannot jump from your spaceship onto a beam of light - even hypothetically - and ask what you would see. It is non-sensical.

You in your spaceship, have a frame of reference in which you are stationary (that's the definition of a FoR). No matter how fast you are moving with respect to any other object in space, you are stationary in your own reference frame, and measure everything around you in that frame.

Light has no reference frame. It can't, because that would entail a reference frame in which it is stationary - which directly contradicts the axiom that light moves at c in all reference frames. It can't be stationbary and moving at c simultaneously.

So there is no "final step". There is massive object and massless objects, and ne'er the twain shall meet.
 
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  • #90
davidjoe said:
but only C (a very specific speed) is claimed to be observed as constant in all reference frames.
Well yes, that is a claim, but so is the claim that there is only one natural number ##N## such that ##2+2=N##. That claim is backed up by a mathematical proof starting from the axioms of number theory, but of course you don't need a lot of advanced mathematics to satisfy yourself that ##2+2=4## and never anything else.

Likewise it has been mathematically proven that either there is no invariant speed, or if there is, then there is exactly one. And likewise, you don't need the math to satisfy yourself of this - just assume that there are two, play around with various objects moving at various speeds relative to one another and greater or less than one or both of your hypothetical invariant speeds, and you will quickly arrive at a contradiction.

So the question has always been whether there is no invariant speed, in which case we have Galilean relativity and velocities add as ##w=u+v##; or there is one invariant speed, in which case we have Einstein's relativity and velocities add according to ##w=(u+v)/(1+uv)##. (And note that the "very specific speed" doesn't show up in this formula at all because I've sensibly chosen units in which the invariant speed is unity).

It's actually something of an accident of history that we call the invariant speed "the speed of light" and represent it with the same symbol ##c## that we used for the measured speed of light. A more modern view would be that there is an invariant speed and the interesting question about light speed is whether light moves at that speed, or at some speed so close to it that our most sensitive measurements have been unable to find any difference.
 
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  • #91
Nugatory said:
Some of your difficulty with relativity may come from not fully appreciating how this description is incorrect (or more precisely, includes a hidden assumption that is incorrect). It makes no sense to talk about the speed of the ship being more or less than the speed of the missile - all we can talk about is the speed of the ship relative to the missile and its negative, which will be the speed of the missile relative to the ship.

The missile is introduced only to illustrate a certain contrast.

Neither your ship nor the missile can attain light speed but are not prevented from traveling just under it.

The purpose of the missile is simply to relate that an object ever-so-close to the speed C, can be in your view eternally, basically.

However, add that tiniest additional speed, the delta between the missile and light, which brings to bear the laser, and now that thinnest of differences in velocity results in seeing a velocity difference of, the speed of light.

In the first thread I posted, if I remember correctly, many pages over many days, it was stated by a member that we no longer use infinite mass in relativity to represent what happens to matter at light speed. But I believe in AE’s time, infinite quantity may have been a nonnegotiable.

To my mind’s thinking, if infinite mass is problem, and I for one think so, (and have since school) such a distinct line between two particular speeds that are virtually identical, may also be.
 
  • #92
Nugatory said:
Well yes, that is a claim, but so is the claim that there is only one natural number ##N## such that ##2+2=N##. That claim is backed up by a mathematical proof starting from the axioms of number theory, but of course you don't need a lot of advanced mathematics to satisfy yourself that ##2+2=4## and never anything else.

Likewise it has been mathematically proven that either there is no invariant speed, or if there is, then there is exactly one. And likewise, you don't need the math to satisfy yourself of this - just assume that there are two, play around with various objects moving at various speeds relative to one another and greater or less than one or both of your hypothetical invariant speeds, and you will quickly arrive at a contradiction.

So the question has always been whether there is no invariant speed, in which case we have Galilean relativity and velocities add as ##w=u+v##; or there is one invariant speed, in which case we have Einstein's relativity and velocities add according to ##w=(u+v)/(1+uv)##. (And note that the "very specific speed" doesn't show up in this formula at all because I've sensibly chosen units in which the invariant speed is unity).

It's actually something of an accident of history that we call the invariant speed "the speed of light" and represent it with the same symbol ##c## that we used for the measured speed of light. A more modern view would be that there is an invariant speed and the interesting question about light speed is whether light moves at that speed, or at some speed so close to it that our most sensitive measurements have been unable to find any difference.

To your last paragraph, the only logical answer is that the particular “speed” is what is invariant, not what speed light goes, in my opinion. Particularly, again my opinion, it’s that speed which represents 100% of that which is attainable, and it happens to be that electromagnetic radiation fills that position, alone.
 
  • #93
@davidjoe in 91 posts you have not shown a single line of math. Without math you are just waving your hands, and nobody else can have any precise understanding of what you are talking about. Physics is not done in vague ordinary language. It's done in math.

Here's what the math you need to do should include: pick an inertial frame (the easiest would be the one in which the laser's target is at rest, but if you prefer to use one in which the target is moving at 0.99999c, be my guest, the laws of physics are invariant); write down the equation of the worldline of the laser pulse and the equation of the worldline of the target; find where they intersect; and then search for any path from anywhere on the laser pulse worldline that (a) is not spacelike, and (b) intersects the target worldline before the laser pulse worldline does. After you have failed at enough attempts to find such a path, perhaps you will see why it is impossible. But you will not see it by continuing to concoct more and more complicated assemblages of vague ordinary language.
 
  • #94
davidjoe said:
the only logical answer is that the particular “speed” is what is invariant, not what speed light goes, in my opinion.
This is quite correct--and entirely irrelevant to the question you are struggling with in this thread.
 
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  • #95
davidjoe said:
However, add that tiniest additional speed, the delta between the missile and light, which brings to bear the laser, and now that thinnest of differences in velocity results in seeing a velocity difference of, the speed of light.
Are you confusing the closing speed between two things with the velocities of the two things?

I consider myself to be at rest. A ship passes me moving at speed .99999c.

That ship emits a flash of light in the direction of its travel. I will measure (the question of how I perform these measurements is irrelevant here, but also not trivial) that the flash of light is moving at speed c relative to me. I will measure that the flash of light is gaining on the ship at speed .00001c, calculated by subtracting the forward speed of the ship from the forward speed of the light.

The ship also launches a missile in the direction of travel. Say that this missile moves at speed .5c (relative to its launcher, of course). I will measure its speed to be .9999967c. So how fast is the light gaining on the missile? It's .0000033c, the forward speed of the light minus the forwards speed of the missile. How fast is the missile gaining on the ship? It's the forward speed of the missile minus the forward speed of the ship.

So we aren't treating the speed of light differently here - it adds and subtracts just like the subluminal speeds of the ship and the missile. Relativistic corrections only come in when we add speeds measured in different frame (here the .5c of the missile using a frame in which the ship is at rest and the .99999c speed of the ship using a frame in which I am rest); then we must use the relativistic velocity addition formula which also does not treat the speed of a flash of light differently than the speed of anything else.
 
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  • #96
I’ll come back. Client stuff.
 
  • #97
davidjoe said:
The final step up could be an inch a year, or infinitely smaller than that.

davidjoe said:
The missile is introduced only to illustrate a certain contrast.

davidjoe said:
To your last paragraph, the only logical answer is that the particular “speed” is what is invariant, not what speed light goes, in my opinion. Particularly, again my opinion, it’s that speed which represents 100% of that which is attainable, and it happens to be that electromagnetic radiation fills that position, alone.
You really are desperate not to be wrong. But you are. No amount of analogies and arm waving will make Einstein's Special Relativity fit your daft idea. Learn some maths and then read Einstein's own Book on Special Relativity. It is not hard to follow what he says (if you are not convinced he's wrong.
 
  • #98
davidjoe said:
To your last paragraph, the only logical answer is that the particular “speed” is what is invariant, not what speed light goes, in my opinion. Particularly, again my opinion, it’s that speed which represents 100% of that which is attainable, and it happens to be that electromagnetic radiation fills that position, alone.
If by "that speed" you mean the invariant velocity, then yes, of course, everyone has understood that for many decades.
It's a distinction without a difference though, if light also moves at that invariant speed and there are many good reasons to think that it does.
One hand-waving but fairly convincing argument is that we can calculate the speed of light directly from the laws of electricity and magnetism; these laws are the same in all frames so yield the same speed in all frames. So we expect that the speed of light will be invariant, and we've established by other means that there can be only one invariant speed, so we conclude that either something is wrong with our understanding of E&M or the speed of light and the invariant speed are necessarily the same.

Note 1: The invariant velocity shows up in contexts other than electromagnetic waves. Gravitational waves propagate at that speed, and it is a key element of relativistic quantum field theories, even though these have nothing that we would recognize as a "speed".

Note 2: Were it to turn out that light does not move at the invariant velocity, the metrologists would have to look long and hard at the definition of the meter. We wouldn't have taken this chance if there was any realistic possibility of this happening.
 
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  • #99
We will be talking.
 

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  • #100
sophiecentaur said:
Learn some maths and then read Einstein's own Book on Special Relativity. It is not hard to follow what he says (if you are not convinced he's wrong.
@davidjoe, you should also try a more modern textbook. This is an “as well as” not an “instead of” recommendation (although if you’re only going to do one, it should be the modern one), and Taylor and Wheeler’s “Spacetime Physics” which is available free from https://www.eftaylor.com/spacetimephysics/ is my first choice.

Einstein developed special relativity 120 years ago starting with the perspective of a turn-of-the-last-century physicist, as opposed to that of a motivated 21st century student. Since then generations of physicists have built on that work, corrected some wrong turns, and starting with Hermann Minkowski enormously strengthened and simplified the presentation of the underlying principles.
 
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  • #101
While it is a military consideration rather than a physics consideration, often prior to firing a laser that would blast you out of the universe, there would be light other than the killing laser itself that would be emitted as the laser device warms up to fire, that would be visible briefly before the laser that is fired itself arrives.
 
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  • #102
ohwilleke said:
While it is a military consideration rather than a physics consideration, often prior to firing a laser that would blast you out of the universe, there would be light other than the killing laser itself that would be emitted as the laser device warms up to fire, that would be visible briefly before the laser that is fired itself arrives.
Actually, I can feel the infrared glow of incoming fire love missives even before the “post reply” button gets hit. AE was a really likable, humble man. I’m that far in.
 
  • #103
Nonsense thread is closed for Moderation...

Update -- thread is not working in either the SciFi forum or the technical forums, so it will remain closed.
 
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