Are Space-like and Time-like Vectors Related in Orthogonality?

  • Thread starter Thread starter spaghetti3451
  • Start date Start date
  • Tags Tags
    Vectors
Click For Summary

Homework Help Overview

The discussion revolves around proving relationships between time-like, space-like, and null vectors in the context of four-vectors in special relativity. The original poster presents two statements to prove regarding the nature of vectors when certain conditions are met, specifically focusing on orthogonality and the implications of the 'mostly minus' convention.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore various reference frames to justify the relationships between the vectors. They discuss the implications of the conditions given in the problem statements and question the assumptions made regarding the components of the vectors.

Discussion Status

There is an ongoing exploration of the proofs, with some participants suggesting alternative approaches and questioning the validity of certain assumptions. Guidance has been offered regarding the need for generality in the proofs, and there is recognition of the importance of addressing sign issues in the relationships between the vectors.

Contextual Notes

Participants note that the original problem statements impose specific conditions on the vectors, and there is a discussion about the implications of these conditions on the nature of the vectors involved. The conversation reflects a careful consideration of the mathematical framework and conventions used in the problem.

spaghetti3451
Messages
1,311
Reaction score
31

Homework Statement



Prove the following:

a) If ##P^a## is time-like and ##P^{a}S_{a}=0##, then ##S^{a}## is space-like.

b) If ##P^a## is null and ##P^{a}S^{a}=0##, then ##S_{a}## is space-like or ##S^{a} \propto P^{a}##.

Homework Equations



Using the 'mostly minus' convention, ##A^a## is time-like, null and space-like if ##A^{a}A_{a}## is ##>0,=0, <0## respectively.

The Attempt at a Solution



a) ##S^{a}S_{a} = S^{a}S_{a} + P^{a}S_{a} = (S^{a} + P^{a})S_{a} = (S^{a} + P^{a})(S_{a} + P_{a}) = S^{a}S_{a} + P^{a}S_{a} + P_{a}S^{a} + P^{a}P_{a} = S^{a}S_{a} + P^{a}P_{a} = ?##
 
Physics news on Phys.org
failexam said:
a) ##S^{a}S_{a} = S^{a}S_{a} + P^{a}S_{a} = (S^{a} + P^{a})S_{a} = (S^{a} + P^{a})(S_{a} + P_{a}) ##

How do you justify the last equality shown above?

Note that ##P^{a}S_{a}## is an invariant. It has the same value in all reference frames. Try to pick a nice reference frame using what you know about ##P^{a}##.
 
Well, in the 'mostly minus' convention, ##P^{a} = \{1,0,0,0 \}## is one possibility.

Therefore, ##P^{a}S_{a} = 0## implies ##S_{0} = 0##.

Therefore, ##S^{a}S_{a} = S^{0}S_{0} + S^{1}S_{1} + S^{2}S_{2} + S^{3}S_{3} = S^{1}S_{1} + S^{2}S_{2} + S^{3}S_{3} = - S_{1}S_{1} - S_{2}S_{2} - S_{3}S_{3}##.

##S_{i}S_{i} >0##, so that ##S^{a}S_{a} < 0##, therefore ##S^{a}## is space-like.
 
b) In the 'mostly minus' convention, ##P^{a} = \{-1,-1,0,0 \}## is one possibility.

Therefore, ##P^{a}S_{a} = 0## implies ##S_{0}+S_{1} = 0##, so that ##S^{0}=S_{0}=-S_{1}##.

Therefore, ##S^{a}S_{a} = S^{0}S_{0} + S^{1}S_{1} + S^{2}S_{2} + S^{3}S_{3} = S_{1}S_{1} - S_{1}S_{1} - S_{2}S_{2} - S_{3}S_{3} = - S_{2}S_{2} - S_{3}S_{3}##.

##S_{i}S_{i} >0##, so that ##S^{a}S_{a} < 0##, therefore ##S^{a}## is space-like.

The other possibility is that ##P^{a} \propto S^{a}## for obvious reasons.
 
Are my solutions correct?
 
failexam said:
Well, in the 'mostly minus' convention, ##P^{a} = \{1,0,0,0 \}## is one possibility.

Yes, it's a possibility. But you want a general proof. You have the right idea, but you can't assume that P0 = 1 in the frame where all the Pi = 0. Similarly for part (b) where you assumed that P0 and P1 are both equal to -1.
 
In that case, does ##P^{a} = \{p,0,0,0\}## for part (a) and ##P^{a}=\{p,-p,0,0\}## for part (b) qualify as four-vectors sufficiently general to give a general proof?
 
failexam said:
In that case, does ##P^{a} = \{p,0,0,0\}## for part (a) and ##P^{a}=\{p,-p,0,0\}## for part (b) qualify as four-vectors sufficiently general to give a general proof?
OK. For part (b), you could rotate the spatial coordinate axes to get ##P^{a}=\{p,p,0,0\}## (without any negative signs). But I think the way you wrote it is OK also.

In post 4 you had
failexam said:
b) In the 'mostly minus' convention, ##P^{a} = \{-1,-1,0,0 \}## is one possibility.

Therefore, ##P^{a}S_{a} = 0## implies ##S_{0}+S_{1} = 0##, so that ##S^{0}=S_{0}=-S_{1}##.

Therefore, ##S^{a}S_{a} = S^{0}S_{0} + S^{1}S_{1} + S^{2}S_{2} + S^{3}S_{3} = S_{1}S_{1} - S_{1}S_{1} - S_{2}S_{2} - S_{3}S_{3} = - S_{2}S_{2} - S_{3}S_{3}##.

##S_{i}S_{i} >0##, so that ##S^{a}S_{a} < 0##, therefore ##S^{a}## is space-like.

Logically, can you really claim that ##S^{a}S_{a} < 0## follows from what you have written? Or should you conclude only that ##S^{a}S_{a} \leq 0##?
 
Yes, that proves that ##S^{a}## is space-like or null for part (b)?

But, by the same token, can we also not conclude that ##S^{a}## is space-like or null (and not just space-like) for part (a)?
 
  • #10
failexam said:
Yes, that proves that ##S^{a}## is space-like or null for part (b)?
Yes. Also, you should go on to show that if S is null, then it must be proportional to P.

But, by the same token, can we also not conclude that ##S^{a}## is space-like or null (and not just space-like) for part (a)?
No, you should be able to prove that in (a), S must be space-like. It can't be null. [Of course, S is assumed to be a nonzero 4-vector in both (a) and (b).]
 
  • #11
TSny said:
Yes. Also, you should go on to show that if S is null, then it must be proportional to P.

For the case when both ##S^{a}S_{0}=0## and ##P^{a}P_{a}=0##, there are probably many solutions that relate ##S^{a}## and ##P^{a}##, but one of them is surely ##S^{a}=cP^{a}##. What are the other solutions that could arise?

TSny said:
No, you should be able to prove that in (a), S must be space-like. It can't be null. [Of course, S is assumed to be a nonzero 4-vector in both (a) and (b).]

Ah! If ##S^{a}## is a non-zero four vector in (a), then ##S_{i}S_{i}>0## in (a). Got it!
 
  • #12
failexam said:
For the case when both ##S^{a}S_{0}=0## and ##P^{a}P_{a}=0##, there are probably many solutions that relate ##S^{a}## and ##P^{a}##, but one of them is surely ##S^{a}=cP^{a}##. What are the other solutions that could arise?
You need to show that there are no other solutions when S is null. That is, if S and P are null and ##P^{a}S_{a}=0##, then show that S must be proportional to P.
 
  • #13
Well, ##S^{a}S_{a}=0## means that ##(S_{0})^{2}=(\vec{S})^{2}## and ##P^{a}P_{a}=0## means that ##(P_{0})^{2}=(\vec{P})^{2}##.

Now, let's divide and obtain ##\frac{(S_{0})^{2}}{(P_{0})^{2}} = \frac{(\vec{S})^{2}}{(\vec{P})^{2}}##.

Call the ratio ##\frac{(S_{0})^{2}}{(P_{0})^{2}} = c^{2}##.

Therefore, ##c^{2} = \frac{(\vec{S})^{2}}{(\vec{P})^{2}} \implies (\vec{S})^{2} = c^{2} (\vec{P})^{2}##.

Therefore, component-wise, the four-vectors are proportional.

Is this correct?
 
  • #14
failexam said:
Well, ##S^{a}S_{a}=0## means that ##(S_{0})^{2}=(\vec{S})^{2}## and ##P^{a}P_{a}=0## means that ##(P_{0})^{2}=(\vec{P})^{2}##.

Now, let's divide and obtain ##\frac{(S_{0})^{2}}{(P_{0})^{2}} = \frac{(\vec{S})^{2}}{(\vec{P})^{2}}##.

Call the ratio ##\frac{(S_{0})^{2}}{(P_{0})^{2}} = c^{2}##.

Therefore, ##c^{2} = \frac{(\vec{S})^{2}}{(\vec{P})^{2}} \implies (\vec{S})^{2} = c^{2} (\vec{P})^{2}##.
OK.

Therefore, component-wise, the four-vectors are proportional.
You have not shown that the individual components of S are proportional to the corresponding individual components of P (with the same proportionality constant). For example, everything you stated above could be satisfied with ##(P^0, P^1, P^2, P^3) = (5, 0, 3, 4)## and ##(S^0, S^1, S^2, S^3) = (5, 0, 5, 0)##.

Note that you did not use ##P^aS_a = 0## in your argument above.
 
  • #15
Alright, let me start from scratch.

I need to show that if ##S^{a}## and ##P^{a}## are null, and if ##P^{a}S_{a} = 0##, then ##S^{a} \propto P^{a}##.

Here's my proof.

##S^{a}## is null ##\implies (S_{0})^{2}=(\vec{S})^{2}##.
##P^{a}## is null ##\implies (P_{0})^{2}=(\vec{P})^{2}##.

##P^{a}S_{a}=0 \implies P_{0}S_{0}=(\vec{P}\cdot{\vec{S}}) \implies \sqrt{(\vec{P})^{2}(\vec{S})^{2}}=(\vec{P}\cdot{\vec{S}})##.

Alluding to the rule for dot product in Euclidean geometry, ##P^{i} = k S^{i}## for ##i=1,2,3##, where ##k## is a positive real number.

Therefore, ##(\vec{P})^{2} = k^{2} (\vec{S})^{2} \implies (P_{0})^{2} = k^{2} (S_{0})^{2} \implies P_{0}=kS_{0}##.

What do you think?
 
  • #16
failexam said:
##S^{a}## is null ##\implies (S_{0})^{2}=(\vec{S})^{2}##.
##P^{a}## is null ##\implies (P_{0})^{2}=(\vec{P})^{2}##.

##P^{a}S_{a}=0 \implies P_{0}S_{0}=(\vec{P}\cdot{\vec{S}}) \implies \sqrt{(\vec{P})^{2}(\vec{S})^{2}}=(\vec{P}\cdot{\vec{S}})##.
In getting to the last equation, can you assume that ##P_{0}S_{0} = \sqrt{(\vec{P})^{2}(\vec{S})^{2}}## or only that ##P_{0}S_{0} = \pm \sqrt{(\vec{P})^{2}(\vec{S})^{2}}##?

Alluding to the rule for dot product in Euclidean geometry, ##P^{i} = k S^{i}## for ##i=1,2,3##, where ##k## is a positive real number.
Does ##k## necessarily have to be positive?

Therefore, ##(\vec{P})^{2} = k^{2} (\vec{S})^{2} \implies (P_{0})^{2} = k^{2} (S_{0})^{2} \implies P_{0}=kS_{0}##.

From this argument, you can only conclude that ##P_{0}= \pm kS_{0}##.

What do you think?

I like this approach. It does not require going to a specific reference frame. You just need to take care of the sign issue.

You can use this approach to also prove part (a) without using a specific frame.
 
  • #17
TSny said:
In getting to the last equation, can you assume that ##P_{0}S_{0} = \sqrt{(\vec{P})^{2}(\vec{S})^{2}}## or only that ##P_{0}S_{0} = \pm \sqrt{(\vec{P})^{2}(\vec{S})^{2}}##?

Well, ##(S_{0})^{2}=(\vec{S})^{2} \implies S_{0} = \pm \sqrt{\vec{S}^{2}}## and ##(P_{0})^{2}=(\vec{P})^{2} \implies P_{0} = \pm \sqrt{\vec{P}^{2}}##.

Therefore, ##P_{0}S_{0} = \sqrt{(\vec{P})^{2}(\vec{S})^{2}}##, don't you think?
 
  • #18
failexam said:
Well, ##(S_{0})^{2}=(\vec{S})^{2} \implies S_{0} = \pm \sqrt{\vec{S}^{2}}## and ##(P_{0})^{2}=(\vec{P})^{2} \implies P_{0} = \pm \sqrt{\vec{P}^{2}}##.

Therefore, ##P_{0}S_{0} = \sqrt{(\vec{P})^{2}(\vec{S})^{2}}##, don't you think?
The ##\pm## sign in ##S_{0} = \pm \sqrt{\vec{S}^{2}}## is not necessarily "correlated" with the ##\pm## sign in ##P_{0} = \pm \sqrt{\vec{P}^{2}}## .

There is no reason why ##P_{0}S_{0}## must be positive.
 
  • #19
Let ##P^{i}=cS^{i}##, where ##c## is a non-zero real number.

Therefore, ##P^{a}S_{a}=0 \implies P^{0}S_{0}+P^{i}S_{i} =0 \implies P^{0}S_{0}+cS^{i}S_{i} = 0 \implies P^{0}S_{0}-cS_{i}S_{i} = 0 \implies P^{0}S_{0}-c(S_{0})^{2}=0 \implies S_{0}(P_{0}-cS_{0})=0 \implies S_{0}=0\ \text{or}\ P_{0}=cS_{0} \implies S_{0}=0\ \text{or}\ P^{0}=cS^{0}##.

Now, ##S_{0}=0 \implies (\vec{S})^{2} = (S_{0})^{2}=0##, but ##S^{a}## cannot be a zero vector.

Therefore, ##P^{a} \propto S^{a}##.

Is this correct?
 
  • #20
That looks good to me.
 

Similar threads

Replies
5
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 10 ·
Replies
10
Views
5K
  • · Replies 2 ·
Replies
2
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K