quantumdude
Staff Emeritus
Science Advisor
Gold Member
- 5,560
- 24
geistkiesel said:OK plot a circle in front of you with a diameter with arrows pointing outward, in the direction of expansion, just like we discussed. Now draw a radius rotated say 4 degrees from one of the radii already drawn.
OK, so let the radius along the +y-axis be:
r1(t)=ctj,
and let the radius along the -y-axis be:
r2(t)=-ctj.
Then let a third radius be rotated from the first one by an angle θ, so it is:
r3(t)=(ct)sin(θ)i+(ct)cos(θ)j.
Connect this rotated radius tip to the radius tip farthest back (should look like a shortened diameter).
The vector joining r2 and r3 is:
r32(t)=r2(t)-r3(t)=
r32(t)=-(ct)sin(&theta)i-ct(cos(θ) +1)j.
What is the expansion rate of these radii?
The rate of change of this vector is:
r32'(t)=-c(sin(θ))i-c(cos(θ)+1)j
and the norm is:
|r'32(t)|=[2cos(θ)+2]1/2c, which for small angles is slightly less than 2c, as expected.
If oppositely directed radii are expanding at a 2c rate then slightly off "direclty opposite" radii should conform to the same logic should it not?
Yes, indeed it does.
Aren't all radii expanding with the same logic even though the velocity of expansion, v(e) < c for nonparallel radii? Are we still outside the Lorentz transformaion tho v(e) < c?
We would still be outside the domain of applicability of SR if we tried to Lorentz boost to one of the photons' rest frames, because SR says that photons don't have rest frames.
If so when, if ever , does SR enter this scenario?
It enters when we switch from one frame to another.
Last edited: