Please try putting this in a mathematical form, so I can point out your errors.
You didn't even try. Stop dodging.
Please try putting this in a mathematical form, so I can point out your errors.
I have hilighted the salient key words and phrases for you, seeing as how you seem to have missed them the first time around (again)Originally Posted by Trippy
Because, as you have stated repeatedly, zero angles are preserved by relativistic aberation, but, IIRC as v APPROACHES c, NON-zero angles are still NON zero - they may APPROACH zero, but they are still NON-zero..
You didn't even try. Stop dodging.
Frankly, I am not interested in your bed time stories, if you can't write proper math, there is no way of falsifying your statements.
Here's the prose version, Tach. Do try and follow it.
I have a mirrored pipe, of zero thickness.
Its C[sub]n[/sub] axis is stationary, but the pipe is rotating around it IE we are in the rest frame of the axis (but not co-rotating).
I pause the rotation, at some arbitrary point, and measure its position relative to the axle to be $$(r_1,\theta_1)$$ where r is the radius of our pipe, and $$\theta$$ is the angle of rotation.
I then rotate it through an angle of $$2\pi$$ radians, with an angular velocity of $$\omega$$, and measure it's position again $$(r_2,\theta_2)$$. Performing the neccessary vector addition, I find that the point I am interested in has moved with a displacement of 2r in a time of $$\frac{2\pi}{\omega}$$ seconds, along a vector that is oriented $$\theta_1 +\pi$$ radians from the vertical.
Q.E.D.
I also find that this vector is perpendicular to the tangents representing the mirror plane at both points.
Pete said:An observer in a train watches the ground passing by, and notes that the ground's velocity is parallel to the ground itself.
Do you agree?
An observer in an elevator watches the ground falling away, and notes that the ground's velocity is perpendicular to the ground.
Do you agree?
Tach appears to be claiming that Pete's surface A in post #2 of this thread makes the same angle with the x and x' axes, where the primed frame moves parallel to the x axis.
If so, clock this one up as another basic error by Tach.
Before we proceed further, I reproduce my post unedited and in full:Ok,
I had a look, it is all nonsense.
Here's the prose version, Tach. Do try and follow it.
I have a mirrored pipe, of zero thickness.
Its C[sub]n[/sub] axis is stationary, but the pipe is rotating around it IE we are in the rest frame of the axis (but not co-rotating).
I pause the rotation, at some arbitrary point, and measure its position relative to the axle to be $$(r_1,\theta_1)$$ where r is the radius of our pipe, and $$\theta$$ is the angle of rotation.
I then rotate it through an angle of $$2\pi$$ radians, with an angular velocity of $$\omega$$, and measure it's position again $$(r_2,\theta_2)$$. Performing the neccessary vector addition, I find that the point I am interested in has moved with a displacement of 2r in a time of $$\frac{2\pi}{\omega}$$ seconds, along a vector that is oriented $$\theta_1 +\pi$$ radians from the vertical. I also find that this vector is perpendicular to the tangents representing the mirror plane at both points.
Q.E.D.
Yes, I'm aware of that.What you are being asked to figure out is what happens to an infinitely small portion of the tangent plane to the circumference...
Well, that's your term for it, I can think of better, less ambiguous terms....(the piece that we call a microfacet)...
Again, I'm aware of that.when the wheel rolls an infinitely small amount of time $$dt$$.
No, this is only true in one reference frame, the non-rotating, co-moving reference frame of the axel.Since the motion of the mirror happens to coincide with the tangential velocity in all frames, according to the theory of the Doppler effect, there will be a null shift.
No, that is not what I did. This is what I did:What you did is totally irrelevant, you turned the wheel by $$2 \pi$$ and you claimed that the point under study advanced by $$2r$$ in the direction of the motion of the axle.
...we are in the rest frame of the axis (but not co-rotating)...
I didn't deal with the x component of the velocity. I dealt with the component of the velocity of a point on the circumference of your wheel, that is perpendicular to the plane of the tangent at that point. I then demonstrated how it was non zero in the rest frame of the axel, thus demonstrating according to Pauli's reasoning, which you have accepted, that it must show some doppler shift.From that, you conclude that there is an x component to the velocity (many others have noticed this before you).
I dealt with neither the x component, nor the y component.There is also a y component to velocity. As long as the velocity and the tangent to the surface are colinear, there is zero Doppler effect.
I didn't deal with the x component of the velocity. I dealt with the component of the velocity of a point on the circumference of your wheel, that is perpendicular to the plane of the tangent at that point. I then demonstrated how it was non zero in the rest frame of the axel, thus demonstrating according to Pauli's reasoning, which you have accepted, that it must show some doppler shift.
I dealt with neither the x component, nor the y component.
Please try putting this in a mathematical form, so I can point out your errors.
You are completely predictable Tach.., and absolutely hilarious!
What you are being asked to figure out is what happens to an infinitely small portion of the tangent plane to the circumference (the piece that we call a microfacet)...
Good job! But this is not how the microfacet moved, this is how a point on the circumference moves after a complete rotation.
Tach said:James R said:Tach appears to be claiming that Pete's surface A in post #2 of this thread makes the same angle with the x and x' axes, where the primed frame moves parallel to the x axis.
If so, clock this one up as another basic error by Tach.
Nope, not at all.
Pete said:An observer in a train watches the ground passing by, and notes that the ground's velocity is parallel to the ground itself.
Do you agree?
An observer in an elevator watches the ground falling away, and notes that the ground's velocity is perpendicular to the ground.
Do you agree?
Yes, but I'm still struggling to make out a completely consistent theme in what you're saying.Tangent to the surface. We have been talking about this for hundreds of posts.
I don't believe you have ever addressed my derivation of $$theta'_A$$. If I'm wrong, I apologize, and can you please quote what you said.I already did, several times, starting with post 5. You insist that there isn't so we reached an impasse.
Not at all. Well, that clears that up.
Tell me. Can you answer the two questions below? They seem a lot simpler to me, but you seem to find them unbearably difficult.
No ideas?
When you say tangent to the ground, I'm thinking a displacement vector between two simultaneous events on the ground.
Is that what you mean?
I don't believe you have ever addressed my derivation of $$theta'_A$$. If I'm wrong, I apologize, and can you please quote what you said.
Is there a mistake in the following? If so, where?
A is defined by:
$$y = x \tan(\theta_A)$$
Transforming A, we find:
$$y' = \gamma\tan(\theta_A) (x' + vt')$$
The angle between A' and the x'-axis is therefore:
$$\tan(\theta'_A) = \gamma\tan(\theta_A)$$
And now a more formal approach.
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Consider a flat surface A in inertial motion in a 2+1 spacetime.
Choose an inertial reference frame S(x,y,t), such that in S:
- A is at rest.
- The angle between the surface A and the x-axis is $$\theta_A$$.
- A intersects (x,y,t)=(0,0,0)
A is thus defined by:
$$y = x \tan(\theta_A)$$
An inertial particle P passes through (x,y,t)=(0,0,0) with velocity $$\vec{V_p}$$.
The angle between $$\vec{V_p}$$ and the x-axis is $$\theta_P$$.
The worldline of P is thus defined by:
$$\begin{align}
x &= t |\vec{V_p}| \cos(\theta_P) \\
y &= t |\vec{V_p}| \sin(\theta_P)
\end{align}$$
You would benefit from checking the answers before you start trolling.