Relativistic Doppler Shift and a Star breaking up

AI Thread Summary
The discussion revolves around calculating the velocities and angles of two remnants from a star that has broken apart, using the relativistic Doppler shift equations. The initial frequency of the star is given, and the frequencies of the remnants are provided, leading to the need to establish relationships between their velocities and angles. The participants engage in deriving equations based on the Doppler effect, emphasizing the importance of conservation of momentum and the angles involved. A significant issue arises when the calculations suggest an impossible negative value for beta, indicating a potential error in the provided data or calculations. The conversation concludes with a call to re-evaluate the equations and assumptions made throughout the problem-solving process.
  • #51
Looks OK.
 
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  • #52
So now:

\frac{7.135}{(\frac{6.690}{1-\beta^2})} = -\frac{ 4.282}{(\frac{6.690}{1-\beta^2})} + 2

And:

((1-\beta^2) \frac{7.135}{6.690})}) = -((1-\beta^2)(\frac{ 4.282}{6.690}) + 2

Does this look okay?

TFM
 
  • #53
Sure. But let's not go through each step. Take it home. Isolate (1 - \beta^2), then solve for \beta. (Show each step, but don't wait for confirmation before continuing.)
 
  • #54
Rght, so

((1-\beta^2) \frac{7.135}{6.690})}) + ((1-\beta^2)(\frac{ 4.282}{6.690}) = 2

Putting the 1 + beta squared on top:

\frac{7.135(1-\beta^2)}{6.690})} + \frac{(1-\beta^2)4.282}{6.690} = 2

Add together:

\frac{7.135(1-\beta^2) + (1-\beta^2)4.282}{6.690})} = 2

Times by 6.690

7.135(1-\beta^2) + (1-\beta^2)4.282 = 2*6.69

11.417(1-\beta^2) = 13.38

So

1-\beta^2 = 13.38/11.417

1-\beta^2 = 1.172

1 = 1.172 + \beta^2

\beta^2 = 1-1.172

\beta^2 = -0.17

I have I done something wrong? you cannot square root a negative number?

TFM
 
  • #55
TFM said:
I have I done something wrong? you cannot square root a negative number?
Remember what I said (in post #35) about there being something wrong with the data? That's what I'm talking about.
 
  • #56
Would the best thing to do in this case be remove the minus sign, and then indicate on my work I have done so and the reason why?

TFM
 
  • #57
TFM said:
Would the best thing to do in this case be remove the minus sign, and then indicate on my work I have done so and the reason why?
What would be the reason why?

I would present your work clearly (and concisely) and show that it leads to impossible results, which indicates that the problem is flawed. (If your instructor thinks the problem is OK, then I'd like to see his solution.)
 
  • #58
Well, the question is worth ten marks, so I thought just make it a magnitude (by squaring then square rooting the negative number) , so that you can still get a answer, but if you think it would be better to leave it as it is, I will do so.

Thanks,

TFM
 
  • #59
Hey,

I was reading this thread and spotted this,

TFM said:
So


\gamma = \frac{1}{1-\beta^2}


TFM

I've probably missed something but shouldn't this be,

\gamma^{2}=\frac{1}{1-\beta^{2}}

or

\gamma = \sqrt{\frac{1}{1-\beta^2}}
 
  • #60
Vuldoraq said:
Hey,

I was reading this thread and spotted this,



I've probably missed something but shouldn't this be,

\gamma^{2}=\frac{1}{1-\beta^{2}}

or

\gamma = \sqrt{\frac{1}{1-\beta^2}}
Absolutely. Good catch!
 
  • #61
Lets see where I went wrong:

\beta( \frac{7.135*10^{14}}{(6.690*10^{14})\gamma} - 1)) = -\beta(\frac{ 4.282*10^{14}}{(6.690*10^{14})\gamma} - 1)

\gamma = \sqrt{\frac{1}{1 - \beta^2}}

So:

\beta( \frac{7.135*10^{14}}{(6.690*10^{14})(\sqrt{\frac{1}{1 - \beta^2}})} - 1)) = -\beta(\frac{ 4.282*10^{14}}{(6.690*10^{14})(\sqrt{\frac{1}{1 - \beta^2}})} - 1)

Also, can't Gamma be expressed as:

\gamma = \frac{1}{\sqrt{1 - \beta^2}}

??

TFM
 
  • #62
Yeah gamma can have that form too, I would have written like that but I couldn't get the latex to do it for me.
 
  • #63
So, first cancel out the exp. and the beta's:

\frac{7.135}{(6.690)\gamma} - 1 = -\frac{ 4.282}{(6.690)\gamma} + 1

Reinsert gamma:

\frac{7.135}{(6.690)(\frac{1}{\sqrt{1 - \beta^2}} )} - 1 = -\frac{ 4.282}{(6.690)({\frac{1}{\sqrt{1 - \beta^2}}} )} + 1

Multiiply out:

\frac{7.135}{(\frac{6.690}{\sqrt{1 - \beta^2}} )} - 1 = -\frac{ 4.282}{({\frac{6.690}{\sqrt{1 - \beta^2}}} )} + 1

Move over the 1:

\frac{7.135}{(\frac{6.690}{\sqrt{1 - \beta^2}} )} = -\frac{ 4.282}{({\frac{6.690}{\sqrt{1 - \beta^2}}} )} + 2

\frac{7.135}{(\frac{6.690}{\sqrt{1 - \beta^2}} )} + \frac{ 4.282}{({\frac{6.690}{\sqrt{1 - \beta^2}}} )} = 2

Does this look okay?

TFM
 
  • #64
This can go to:

\frac{7.135(\sqrt{1 - \beta^2})}{6.690} + \frac{ 4.282( \sqrt{1 - \beta^2})}{6.690}} = 2

get rid of denominator:

7.135(\sqrt{1 - \beta^2}) + 4.282( \sqrt{1 - \beta^2}) = 2*6.690

This can go to:

11.417 (\sqrt{1 - \beta^2}) = 13.38

and:

\sqrt{1 - \beta^2} = 13.38/11.417

\sqrt{1 - \beta^2} = 1.172

so square out the root:

1 - \beta^2 = 1.373

and:

1 - 1.373 = \beta^2

Is the data still wrong, or have I done something wrong, because I now get beta squared as
-0.373

??

TFM
 
  • #65
Your math looks fine, your answer is the same as my own. It's as Doc Al said, the data is wrong. Slightly annoying because I think it makes it impossible to find the angle, as requested in the second part, though I may be wrong.
 
  • #66
Yes, the data is wrong. When I checked it earlier, I used my own calculations (with correct expression for \gamma).
 
  • #67
Hey all,

Is there a possibility that the answer is imaginary because one velocity is the negative of the other?

Vuldoraq
 
  • #68
I finally have the answer sheet for the question:

Quoted from Sheet:

Since the fragments have equal masses, they must have equal velocities. Using the general Doppler shift relation, we find that for one of the fragments

\frac{v prime}{v} = \frac{6.690*10^{-14}}{7.135*10{-14}} = 0.9376 = \gamma - \beta \gamma cos \theta

whereas for the other

\frac{v prime}{v} = \frac{6.690*10^{-14}}{4.282*10{-14}} = 1.562 = \gamma + \beta \gamma cos \theta

Adding these, we obtain 2γ =2.5 so γ =1.25=5/4 and so

\beta^2 = 1 - \frac{1}{\gamma^2} = 1 - \frac{16}{25} = \frac{9}{25}

and therefore

\beta = \frac{3}{5} = 0.6

which gives a velocity of 0.6 × 3×108 = 1.83 × 108 m/s.
Substituting back into the first equation of this part, we find

0.936 = 1.25(1 - 0.6cos \theta)

0.75 = 1 - 0.6cos \theta

cos \theta = \frac{0.25}{0.6}0.4167

and so the angle is θ = 65.4°.

End Sheet Quote

TFM
 
  • #69
Yeah, I really messed this one up big time. I had reversed the primed and unprimed frequencies (mixing up source and observer). D'oh!

My apologies. :redface:
 

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