Sum of two velocities is smaller than the speed of light

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Using the Lorentz transformation from special relativity, we get that the sum of two velocities can be expressed as
$$u=fracu'+v1+fracu'vc^2.$$
Given that $|u'|,|v| le c$, I want to prove that $|u| le c$, ie. that the velocity never exceeds $c$. However I am struggling to produce this bound. I have tried to bound the denominator from above but this produces zero and have tried a case wise approach but this has got me no where either.
real-analysis special-relativity
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up vote
3
down vote
favorite
Using the Lorentz transformation from special relativity, we get that the sum of two velocities can be expressed as
$$u=fracu'+v1+fracu'vc^2.$$
Given that $|u'|,|v| le c$, I want to prove that $|u| le c$, ie. that the velocity never exceeds $c$. However I am struggling to produce this bound. I have tried to bound the denominator from above but this produces zero and have tried a case wise approach but this has got me no where either.
real-analysis special-relativity
add a comment |Â
up vote
3
down vote
favorite
up vote
3
down vote
favorite
Using the Lorentz transformation from special relativity, we get that the sum of two velocities can be expressed as
$$u=fracu'+v1+fracu'vc^2.$$
Given that $|u'|,|v| le c$, I want to prove that $|u| le c$, ie. that the velocity never exceeds $c$. However I am struggling to produce this bound. I have tried to bound the denominator from above but this produces zero and have tried a case wise approach but this has got me no where either.
real-analysis special-relativity
Using the Lorentz transformation from special relativity, we get that the sum of two velocities can be expressed as
$$u=fracu'+v1+fracu'vc^2.$$
Given that $|u'|,|v| le c$, I want to prove that $|u| le c$, ie. that the velocity never exceeds $c$. However I am struggling to produce this bound. I have tried to bound the denominator from above but this produces zero and have tried a case wise approach but this has got me no where either.
real-analysis special-relativity
real-analysis special-relativity
asked 2 hours ago
user258521
328210
328210
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add a comment |Â
4 Answers
4
active
oldest
votes
up vote
4
down vote
accepted
With only basic analysis, you can do it by fixing one of the two variables.
You can prove that, for a fixed $u'<c$:
- The function $f_u'(v)=fracu'+v1+fracu'c^2v$ is a monotonically increasing function.
- $f_u'(c)=c$
From $1$, you can conclude that if $v<c$, $f_u'(v)<f_u'(c)$,and including $2$, that gives you $f_u'(v)<c$.
This proves that if $u',v$ are both smaller than $c$, that $fracu'+v1+fracu'vc^2$ will also be smaller than $c$.
This is very nice !
â user258521
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
add a comment |Â
up vote
1
down vote
Hint: If you're familiar with techniques in optimization, try and choose values of $u'$ and $v$ so as to optimize $u$. If you can prove that the optimal values for making $u$ large yield a value of $u$ at or approaching $c$, then you are done.
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
add a comment |Â
up vote
1
down vote
Here's an elementary general proof.
Letting $x=u'/c, y = v/c, z = u/c$ the equation for the Einstein sum becomes
$$z = fracx+y1+x ytag1$$
and we have to prove that
$$-1lt z lt 1tag2$$
for $-1lt x lt 1, -1 lt y lt 1$.
Now we let
$$xto frac1-r1+r,yto frac1-s1+stag3a$$
or
$$r to frac1-x1+x, sto frac1-y1+ytag3b$$
which transforms $xin (-1,+1)$ to $r in (infty, 0)$ and $yin (-1,+1)$ to $s in (infty, 0)$ .
In other words, we have parametrized $x$ and $y$ with positive parameters $r$ and $s$.
Substituting (3) in (1) gives
$$z = frac1-t1+ttag4$$
with $t = r s$. Hence we have $t in (infty, 0)$ and from (4) follows (2). QED.
add a comment |Â
up vote
0
down vote
Such relativistic sum of speeds (here denoted as $oplus$) can be written in terms of a simple pullback:
$$ uoplus vstackreltextdef=ccdottanhleft(textarctanhtfracuc+textarctanhtfracvcright)$$
since $tanh$ is an increasing function with range $(-1,1)$, $left|uoplus vright|< c$ immediately follows.
add a comment |Â
4 Answers
4
active
oldest
votes
4 Answers
4
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
4
down vote
accepted
With only basic analysis, you can do it by fixing one of the two variables.
You can prove that, for a fixed $u'<c$:
- The function $f_u'(v)=fracu'+v1+fracu'c^2v$ is a monotonically increasing function.
- $f_u'(c)=c$
From $1$, you can conclude that if $v<c$, $f_u'(v)<f_u'(c)$,and including $2$, that gives you $f_u'(v)<c$.
This proves that if $u',v$ are both smaller than $c$, that $fracu'+v1+fracu'vc^2$ will also be smaller than $c$.
This is very nice !
â user258521
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
add a comment |Â
up vote
4
down vote
accepted
With only basic analysis, you can do it by fixing one of the two variables.
You can prove that, for a fixed $u'<c$:
- The function $f_u'(v)=fracu'+v1+fracu'c^2v$ is a monotonically increasing function.
- $f_u'(c)=c$
From $1$, you can conclude that if $v<c$, $f_u'(v)<f_u'(c)$,and including $2$, that gives you $f_u'(v)<c$.
This proves that if $u',v$ are both smaller than $c$, that $fracu'+v1+fracu'vc^2$ will also be smaller than $c$.
This is very nice !
â user258521
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
add a comment |Â
up vote
4
down vote
accepted
up vote
4
down vote
accepted
With only basic analysis, you can do it by fixing one of the two variables.
You can prove that, for a fixed $u'<c$:
- The function $f_u'(v)=fracu'+v1+fracu'c^2v$ is a monotonically increasing function.
- $f_u'(c)=c$
From $1$, you can conclude that if $v<c$, $f_u'(v)<f_u'(c)$,and including $2$, that gives you $f_u'(v)<c$.
This proves that if $u',v$ are both smaller than $c$, that $fracu'+v1+fracu'vc^2$ will also be smaller than $c$.
With only basic analysis, you can do it by fixing one of the two variables.
You can prove that, for a fixed $u'<c$:
- The function $f_u'(v)=fracu'+v1+fracu'c^2v$ is a monotonically increasing function.
- $f_u'(c)=c$
From $1$, you can conclude that if $v<c$, $f_u'(v)<f_u'(c)$,and including $2$, that gives you $f_u'(v)<c$.
This proves that if $u',v$ are both smaller than $c$, that $fracu'+v1+fracu'vc^2$ will also be smaller than $c$.
edited 2 hours ago
answered 2 hours ago
5xum
86.2k388155
86.2k388155
This is very nice !
â user258521
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
add a comment |Â
This is very nice !
â user258521
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
This is very nice !
â user258521
2 hours ago
This is very nice !
â user258521
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
@user258521 Thanks. It's a little strange in the sense that you "break the symmetry" of the original expression - you view one variable as a variable, and the other as a parameter, and then solve the problem for each value of the parameter. Some call it ugly, some like it, it depends. But so long as it works :)
â 5xum
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
I think it is perfectly fine, nothing wrong with this. Also in 1. it should have $c^2$ on the denominator, a small edit.
â user258521
2 hours ago
add a comment |Â
up vote
1
down vote
Hint: If you're familiar with techniques in optimization, try and choose values of $u'$ and $v$ so as to optimize $u$. If you can prove that the optimal values for making $u$ large yield a value of $u$ at or approaching $c$, then you are done.
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
add a comment |Â
up vote
1
down vote
Hint: If you're familiar with techniques in optimization, try and choose values of $u'$ and $v$ so as to optimize $u$. If you can prove that the optimal values for making $u$ large yield a value of $u$ at or approaching $c$, then you are done.
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
add a comment |Â
up vote
1
down vote
up vote
1
down vote
Hint: If you're familiar with techniques in optimization, try and choose values of $u'$ and $v$ so as to optimize $u$. If you can prove that the optimal values for making $u$ large yield a value of $u$ at or approaching $c$, then you are done.
Hint: If you're familiar with techniques in optimization, try and choose values of $u'$ and $v$ so as to optimize $u$. If you can prove that the optimal values for making $u$ large yield a value of $u$ at or approaching $c$, then you are done.
answered 2 hours ago
Cade Reinberger
1527
1527
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
add a comment |Â
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
The only optimisation techniques I can think of are derivatives so not too sure if this will be useful? Relating to your answer, $u'=v=c$ is a possible value but not sure how the argument follows?
â user258521
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
Well, you're optimizing over a square, which importantly is compact. Explicitly, first prove the problem on the boundary (that is, when at least one of $u'$ or $v$ is $c$). Then you know if there is any value above c, it must be on the interior, and thus must be a simultaneous zero of both partial derivatives.
â Cade Reinberger
2 hours ago
add a comment |Â
up vote
1
down vote
Here's an elementary general proof.
Letting $x=u'/c, y = v/c, z = u/c$ the equation for the Einstein sum becomes
$$z = fracx+y1+x ytag1$$
and we have to prove that
$$-1lt z lt 1tag2$$
for $-1lt x lt 1, -1 lt y lt 1$.
Now we let
$$xto frac1-r1+r,yto frac1-s1+stag3a$$
or
$$r to frac1-x1+x, sto frac1-y1+ytag3b$$
which transforms $xin (-1,+1)$ to $r in (infty, 0)$ and $yin (-1,+1)$ to $s in (infty, 0)$ .
In other words, we have parametrized $x$ and $y$ with positive parameters $r$ and $s$.
Substituting (3) in (1) gives
$$z = frac1-t1+ttag4$$
with $t = r s$. Hence we have $t in (infty, 0)$ and from (4) follows (2). QED.
add a comment |Â
up vote
1
down vote
Here's an elementary general proof.
Letting $x=u'/c, y = v/c, z = u/c$ the equation for the Einstein sum becomes
$$z = fracx+y1+x ytag1$$
and we have to prove that
$$-1lt z lt 1tag2$$
for $-1lt x lt 1, -1 lt y lt 1$.
Now we let
$$xto frac1-r1+r,yto frac1-s1+stag3a$$
or
$$r to frac1-x1+x, sto frac1-y1+ytag3b$$
which transforms $xin (-1,+1)$ to $r in (infty, 0)$ and $yin (-1,+1)$ to $s in (infty, 0)$ .
In other words, we have parametrized $x$ and $y$ with positive parameters $r$ and $s$.
Substituting (3) in (1) gives
$$z = frac1-t1+ttag4$$
with $t = r s$. Hence we have $t in (infty, 0)$ and from (4) follows (2). QED.
add a comment |Â
up vote
1
down vote
up vote
1
down vote
Here's an elementary general proof.
Letting $x=u'/c, y = v/c, z = u/c$ the equation for the Einstein sum becomes
$$z = fracx+y1+x ytag1$$
and we have to prove that
$$-1lt z lt 1tag2$$
for $-1lt x lt 1, -1 lt y lt 1$.
Now we let
$$xto frac1-r1+r,yto frac1-s1+stag3a$$
or
$$r to frac1-x1+x, sto frac1-y1+ytag3b$$
which transforms $xin (-1,+1)$ to $r in (infty, 0)$ and $yin (-1,+1)$ to $s in (infty, 0)$ .
In other words, we have parametrized $x$ and $y$ with positive parameters $r$ and $s$.
Substituting (3) in (1) gives
$$z = frac1-t1+ttag4$$
with $t = r s$. Hence we have $t in (infty, 0)$ and from (4) follows (2). QED.
Here's an elementary general proof.
Letting $x=u'/c, y = v/c, z = u/c$ the equation for the Einstein sum becomes
$$z = fracx+y1+x ytag1$$
and we have to prove that
$$-1lt z lt 1tag2$$
for $-1lt x lt 1, -1 lt y lt 1$.
Now we let
$$xto frac1-r1+r,yto frac1-s1+stag3a$$
or
$$r to frac1-x1+x, sto frac1-y1+ytag3b$$
which transforms $xin (-1,+1)$ to $r in (infty, 0)$ and $yin (-1,+1)$ to $s in (infty, 0)$ .
In other words, we have parametrized $x$ and $y$ with positive parameters $r$ and $s$.
Substituting (3) in (1) gives
$$z = frac1-t1+ttag4$$
with $t = r s$. Hence we have $t in (infty, 0)$ and from (4) follows (2). QED.
edited 17 mins ago
answered 40 mins ago
Dr. Wolfgang Hintze
2,785515
2,785515
add a comment |Â
add a comment |Â
up vote
0
down vote
Such relativistic sum of speeds (here denoted as $oplus$) can be written in terms of a simple pullback:
$$ uoplus vstackreltextdef=ccdottanhleft(textarctanhtfracuc+textarctanhtfracvcright)$$
since $tanh$ is an increasing function with range $(-1,1)$, $left|uoplus vright|< c$ immediately follows.
add a comment |Â
up vote
0
down vote
Such relativistic sum of speeds (here denoted as $oplus$) can be written in terms of a simple pullback:
$$ uoplus vstackreltextdef=ccdottanhleft(textarctanhtfracuc+textarctanhtfracvcright)$$
since $tanh$ is an increasing function with range $(-1,1)$, $left|uoplus vright|< c$ immediately follows.
add a comment |Â
up vote
0
down vote
up vote
0
down vote
Such relativistic sum of speeds (here denoted as $oplus$) can be written in terms of a simple pullback:
$$ uoplus vstackreltextdef=ccdottanhleft(textarctanhtfracuc+textarctanhtfracvcright)$$
since $tanh$ is an increasing function with range $(-1,1)$, $left|uoplus vright|< c$ immediately follows.
Such relativistic sum of speeds (here denoted as $oplus$) can be written in terms of a simple pullback:
$$ uoplus vstackreltextdef=ccdottanhleft(textarctanhtfracuc+textarctanhtfracvcright)$$
since $tanh$ is an increasing function with range $(-1,1)$, $left|uoplus vright|< c$ immediately follows.
answered 29 mins ago
Jack D'Aurizioâ¦
278k33272646
278k33272646
add a comment |Â
add a comment |Â
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