Moving light bulb sphere of photons

In summary, the observer inside the moving light bulb would see an expanding sphere of photons when the light is turned on. However, if the observer is outside of the light bulb and moving along the x-axis, the photons will appear to be bent due to the observer's frame of reference. This means that the shape formed by the photons will not be a perfect sphere, but rather a skewed sphere or another shape. This is because the amount of bending is proportional to the angle the photons make with the x-axis. Therefore, the photons cannot form a perfect sphere around the observer.
  • #1
Dreads
69
0
If you have a moving light bulb and an observer at rest wrt the light bulb. The observer is tiny and he is inside the light bulb. The light bulb is traveling along the x axis. The light is then turned on what will the observer see..a sphere of photons traveling outwards from the observer?

Keep in mind if you are in a spaceship traveling in the direction of the x-axis and there is a a laser trained on a spot along the Y axis . Regardless of the velocity of the frame of reference the laser will always remain trained on the spot.

so if the frame goes faster the photons from the laser will "bend" more so they remain on the spot

Therefore photons traveling perpendicular to the direction of travell MUST bend more than non perpendicular photons. The amount a photons bends is propriotional to the angle the photons makes wrt the x axis. Photons traveling along the x-axis will not bend at all.

Therefore the photons cannot form a sphere around the observer as they are not all bending by the same amount. The shape formed wiil be a skewed sphere or a shapes that is NOT an sphere... is there something I am missing here?
 
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  • #2
Yes, you are missing that photons propagate at the same velocity to all observers (assuming that the inside of the light bulb is a vacuum, i.e. there is no argon, neon or nitrogen inside).
 
  • #3
If you are on the light bulb, you see an expanding sphere of photons.
On the other hand, if you are any other observer, you see an expanding sphere of photons.

You are missing that the speed of light is c in all reference frames.

In a frame in which the light bulb is moving, you will also observe doppler shifting and relativistic beaming, but the wavefront is always a sphere.
 
  • #4
ZikZak said:
In a frame in which the light bulb is moving, you will also observe doppler shifting and relativistic beaming, but the wavefront is always a sphere.
It's not only frequence to be different because of the moving frame, but amplitude too, so I can't understand how the wavefront can stay spherical.
 
  • #5
lightarrow said:
It's not only frequence to be different because of the moving frame, but amplitude too, so I can't understand how the wavefront can stay spherical.

The wavefront remains spherical because the speed of light is c. Frequency and amplitude aren't speed.
 
  • #6
ZikZak said:
The wavefront remains spherical because the speed of light is c. Frequency and amplitude aren't speed.
Yes, it's correct, sorry.
 
  • #7
The equation of the sphere of light in the stationary frame is:
c²t² = x² + y² + z²

Transforming to the moving frame is:
(ct'γ-vx'γ/c)² = γ²(x'-vt')² + y'² + z'²

Which simplifies to:
c²t'² = x'² + y'² + z'²
 
  • #8
My animations at
http://physics.syr.edu/courses/modules/LIGHTCONE/LightClock/#circularlightclocks
might help you visualize the situation.

The intersection of
the light rays emitted by an event on an inertial observer's worldline
and the worldtube traced out by a circular array of mirrors around that observer
is, according to that observer,
a set of simultaneous events that are equidistant in space from the observer
(i.e. a circular wavefront).

The analogous situation is constructed for
an inertial observer moving with respect to this first observer.
 
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  • #9
Dreads said:
If you have a moving light bulb and an observer at rest wrt the light bulb. The observer is tiny and he is inside the light bulb. The light bulb is traveling along the x axis. The light is then turned on what will the observer see..a sphere of photons traveling outwards from the observer?

Keep in mind if you are in a spaceship traveling in the direction of the x-axis and there is a a laser trained on a spot along the Y axis . Regardless of the velocity of the frame of reference the laser will always remain trained on the spot.

so if the frame goes faster the photons from the laser will "bend" more so they remain on the spot

Therefore photons traveling perpendicular to the direction of travell MUST bend more than non perpendicular photons. The amount a photons bends is propriotional to the angle the photons makes wrt the x axis. Photons traveling along the x-axis will not bend at all.

Therefore the photons cannot form a sphere around the observer as they are not all bending by the same amount. The shape formed wiil be a skewed sphere or a shapes that is NOT an sphere... is there something I am missing here?

Could he see a sphere of photons traveling outwards?
 
  • #10
DaleSpam said:
The equation of the sphere of light in the stationary frame is:
c²t² = x² + y² + z²

Transforming to the moving frame is:
(ct'γ-vx'γ/c)² = γ²(x'-vt')² + y'² + z'²

Which simplifies to:
c²t'² = x'² + y'² + z'²

... which is rather obvious, because the transformation
ct = ct'γ-vx'γ/c
x = γ(x'-vt')
is derived precisely from the requirement that the speed of light be constant to any observer (i.e. from c²t² = x² + y² + z² holding in any Lorentz-equivalent frame).
 
  • #11
Thanks, DaleSpam, robphy, CompuChip.
 
  • #12
Assume we have the stroy above with the globe moving along the x-axis yadda yadda yadda

so you have the observer at the centre of photons moving out in all directions. Imagine the photons as lines of equal length raditiang from a central point. Imagine for now just in 2D. A perfect analogy is a wagon wheel with lots of spokes. But some of the spokes are straight( the photons moving along the x axis) and some of the spokes are bent with the amount of bending being propotional to the angle the spoke makes with the x axis. Spokes at 90 degrees to the x-axis bend the most.

With some of the spokes straight and others bent, and they are all the same length they will NOT form a circle. Rotate this malformed wagon wheel thru 360 degrees around the x axs and it is not a sphere
 
  • #13
Dreads said:
Imagine the photons as lines of equal length raditiang from a central point.

the lines will be equal length as all photons are moving at C. The wagon wheel analogy is what the photons will look like at a snap shot in time say T0
 
  • #14
Dreads said:
With some of the spokes straight and others bent, and they are all the same length they will NOT form a circle. Rotate this malformed wagon wheel thru 360 degrees around the x axs and it is not a sphere

When I say that the spokes are bent I mean they will not be radiating out from the central point, perpendicular to a tangent of that central point.

if you draw a circle around the central point with the central point as the centre of the circle, the radiating lines will not be perpendicular to the tangent of that circle.

Only the photons moving along the x-axis will be perpendiular to a tangent to the aformetioned circle.
 
  • #15
the only way the spokes of a wagon wheel, bike wheel etc, with equal length spokes, can form a circle is if all the spokes are perpendicular to the tangent to a second circle, where the tangent is taken at the point where the spoke intersects the second circle. With the centre of the second circle being the centre of the spokes.

Move any spoke the tiniest amount away from perpendicular and the spokes will no longer form a perfect circle
 
  • #16
Dreads said:
the only way the spokes of a wagon wheel, bike wheel etc, with equal length spokes, can form a circle is if all the spokes are perpendicular to the tangent to a second circle, where the tangent is taken at the point where the spoke intersects the second circle. With the centre of the second circle being the centre of the spokes.
If all the spokes radiate out from a single center point, they will automatically be tangent to a circle with that point at its center, no? There's no way you could have a bunch of equal-length spokes that all radiate from a single point that don't all end in points on a circle. After all, every radius of a circle is just a straight line segment going from the center to a point on the circle, it's impossible to draw a straight line going from the center that doesn't lie along one of the radial lines.
 
  • #17
Dreads said:
Rotate this malformed wagon wheel thru 360 degrees around the x axs and it is not a sphere
Yes it is a sphere; I derived it above.

Since your conclusion is demonstrably wrong, why don't you go back and see if you can spot the mistake.
 
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  • #18
sorry I apologise you are all right

sorry to labour the point but another thought occurred to me

what will change in a moving frame of reference is the photon density

take my wagon wheel analogy from before
place the axis of the wagon wheel on the origin of a cartesian coordinate system in the xy plane

The wagon wheel is now broken into 4 quadrants by the coor system +x+y,-x+y,-y-x and -y+x

if the spokes of the wagon wheel are evenly spaced in a stationary frame ie 1 spoke every 2 degrees so 180 spokes for the entire circle and each spoke is evenly spaced. So the densitty of the spokes in any given quadrant will be 45 spokes per quadrant. If the spokes were photons same deal

the same wagon wheel in a moving frame the spokes will not be evenly spaced, their density in each quadrant will not be the same.

In a moving frame the photons (spokes) rotate. The photons must rotate to keep the laser on the spot from my riginal post. The photons in the +y half of the circle rotate clockwise, the photons in the -y half of the circle rotate counter clockwise

so for any quadrant spoke(photon) density in stationary frame will be 45
so for any quadrant spoke(photon) density in moving frame will not be 45

I draw this conslusion from the fact that the photons moving perpendicuar to the direction of movement of the frame rotate more than photons at a lesser angle. The amount of rotation will be proprtional to the angle the photon makes with th x axis.

I suspect the rotation is a function of sin(x) as maximum rotation will occur at 90 degrees. Photons moving along the x-axis will not rotate at all


or am I wrong?
 
  • #19
Dreads said:
Assume we have the stroy above with the globe moving along the x-axis yadda yadda yadda

so you have the observer at the centre of photons moving out in all directions. Imagine the photons as lines of equal length raditiang from a central point. Imagine for now just in 2D. A perfect analogy is a wagon wheel with lots of spokes. But some of the spokes are straight( the photons moving along the x axis) and some of the spokes are bent with the amount of bending being propotional to the angle the spoke makes with the x axis. Spokes at 90 degrees to the x-axis bend the most.

With some of the spokes straight and others bent, and they are all the same length they will NOT form a circle. Rotate this malformed wagon wheel thru 360 degrees around the x axs and it is not a sphere
Why would some of the spokes be bent? The path of a photon is always a straight line as seen from an observer at rest with the source or in uniform relative motion.
 
  • #20
Dreads said:
Keep in mind if you are in a spaceship traveling in the direction of the x-axis and there is a a laser trained on a spot along the Y axis . Regardless of the velocity of the frame of reference the laser will always remain trained on the spot.

for the observer within the spaceship to observe the laser on the spot at any velocity the photons from the laser must rotate in the direction of travel. If they didnt then the observer within the spaceship would see the laser move off the spot and he would know he was moving
 
  • #21
Can you derive the equation that describes this rotation?
 
  • #22
no, but i can't derive the equation that describes the sun ether but its there

the photons must rotate otherwise given the laser spot scenario in my inital post it would be trivial for an observer in a MFR at rest wrt that MFR to prove that they were in a MFR. I know it has somthing to do with conservation of momentum and maxwells symmetry
 
  • #23
as I said before it will be a function of the velocity of the MFR and sin(N) where N is the angle the photon makes with the x axis
 
  • #24
Hello Dreads.

Think of it this way. The centre of the expanding sphere of photons is at rest in EVERY frame. So for ANY observers present at the point of emission, no matter what their relative velocities, the expanding sphere of photons behaves as if any and all of the observers are, and remain, central to it. It is non intuitive and makes no "common sense" but it is due to the speed of light being the same in all inertial frames and is at the very heart of relativity.

Matheinste
 
  • #25
Hi Dreads,

The reason I asked is because I don't know what you even mean by the rotation of a photon. Do you picture a photon as some extended rigid body object that spins about some axis, or is it rotating about some external axis, or what?

I was hoping you could describe that mathematically (you don't need to derive it from first principles) so that I could understand what you meant by a photon rotating.
 
  • #26
I think Dreads just means that the angles that each photon is traveling will rotate when you compare the frame moving relative to the source with the source's rest frame--think of the light clock thought experiment, where in the clock's rest frame the photon travels straight up along the y-axis from one mirror to another, but in the frame where the clock is moving the photon travels at an angle to the y-axis.

And if this is what was meant, then I agree with post #18 that if the density of the photons on the light sphere is even in the source's rest frame, then in the frame where the source is moving the density of photons will be higher on one side of the sphere than on the other.
 
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  • #27
JesseM said:
I think Dreads just means that the angles that each photon is traveling will rotate when you compare the frame moving relative to the source with the source's rest frame--think of the light clock thought experiment, where in the clock's rest frame the photon travels straight up along the y-axis from one mirror to another, in the frame where the clock is moving the photon travels at an angle to the y-axis.
Ahh, OK. I thought he meant that the worldline of a photon was not a straight line. That its path curved. I got distracted by the "bent spokes" comment.

Dreads, is JesseM correct? If so then yes, the angle will not be the same in all frames, but straight lines will map to straight lines in all frames.
 
  • #28
DaleSpam said:
but straight lines will map to straight lines in all frames.

I take it this means striagh lines are striagh lines in all frames?
 
  • #29
Dreads said:
I take it this means striagh lines are striagh lines in all frames?
All inertial frames, yes.
 
  • #30
Correct. The Lorentz transform is a linear transform, therefore a straight line in one inertial frame is a straight line in all inertial frames.

JesseM was faster!
 
  • #31
matheinste said:
Hello Dreads.

Think of it this way. The centre of the expanding sphere of photons is at rest in EVERY frame. So for ANY observers present at the point of emission, no matter what their relative velocities, the expanding sphere of photons behaves as if any and all of the observers are, and remain, central to it. It is non intuitive and makes no "common sense" but it is due to the speed of light being the same in all inertial frames and is at the very heart of relativity.

Matheinste

is this for real ?

so what you are saying is if we have three observers, OB1, OB2 (and OBkenobee3 sorry couldn't resist that) Ob3 tarvelling along the x, y and z axis and they all intersect at T0 at the origin of a cartersian coor sys. At the origin is a light bulb that turns on at T0

Ob1 is traveling at seed 1 km/h, 0b2 at 0.5 C and ob3 at c what you are saying is that they will all see the same a sphere of photons expanding outwardly in all directions and each observer will percieve themelves at the centre of the sphere?
 
  • #32
sorry I am a hopeless speller, can't spell striat :)
 
  • #33
Dreads said:
is this for real ?

so what you are saying is if we have three observers, OB1, OB2 (and OBkenobee3 sorry couldn't resist that) Ob3 tarvelling along the x, y and z axis and they all intersect at T0 at the origin of a cartersian coor sys. At the origin is a light bulb that turns on at T0

Ob1 is traveling at seed 1 km/h, 0b2 at 0.5 C and ob3 at c
What are these speeds relative to? The light bulb, perhaps? Keep in mind all speeds are relative in SR. Also, if OB3 is traveling at c, then OB3 does not have his own inertial rest frame, because the only valid inertial frames are ones moving slower than light--maybe we could modify the example so that OB3 is traveling at 0.99c relative to the bulb?
Dreads said:
what you are saying is that they will all see the same a sphere of photons expanding outwardly in all directions and each observer will percieve themelves at the centre of the sphere?
As long as they are inertial observers moving slower than light, then yes, in each of their own inertial rest frames they will remain at the center of the sphere of photons.
 
  • #34
Dreads said:
is this for real ?

so what you are saying is if we have three observers, OB1, OB2 (and OBkenobee3 sorry couldn't resist that) Ob3 tarvelling along the x, y and z axis and they all intersect at T0 at the origin of a cartersian coor sys. At the origin is a light bulb that turns on at T0

Ob1 is traveling at seed 1 km/h, 0b2 at 0.5 C and ob3 at c what you are saying is that they will all see the same a sphere of photons expanding outwardly in all directions and each observer will percieve themelves at the centre of the sphere?

Absolutely correct, except that no observer can travel at c. If we allow that observer to travel at nearly c, then the speed of light is c in all three frames. Therefore, each observer observes a sphere of photons, centered on himself, expanding at speed c.
 

FAQ: Moving light bulb sphere of photons

1. What is a "moving light bulb sphere of photons"?

A moving light bulb sphere of photons is a theoretical concept that describes a light bulb that is emitting photons in all directions while also moving through space.

2. How does the movement of the light bulb affect the photons it emits?

The movement of the light bulb can affect the direction and speed of the photons it emits. This is due to the Doppler effect, which causes the wavelength of the photons to change based on the relative motion between the light source and the observer.

3. Can a light bulb actually emit photons in all directions?

No, a light bulb emits photons in a specific direction based on the design of the bulb and its filament. However, if the bulb is rotating or moving, it may appear to emit photons in all directions due to the changing perspective of the observer.

4. What is the significance of studying a moving light bulb sphere of photons?

Studying a moving light bulb sphere of photons can help us understand the behavior of light and the effects of motion on light. It also has practical applications in fields such as astronomy and engineering.

5. Is a moving light bulb sphere of photons possible in real life?

While a light bulb moving through space and emitting photons is possible, it is unlikely that it would emit photons in all directions. This concept is mostly used in theoretical scenarios to better understand the behavior of light.

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