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Conserving algebraic quantities


How to average cyclic quantities?Factoring Quantities QuestionWhat is $f(x)$ divided by $(x-a)$?Exponential growth on discrete quantitiesProblem finding quantities given ratiosCalculating quantitiesAlgebraic doubt concerning orthogonal polynomials in physics research paperFinding limit for infinite quantities.Why are the number of roots of the characteristic equation of a PDE infinite?Show that $x_n+1 = fracx_n + 1n+1$ is decreasing starting from some $n_0$ and find $n_0$.













1












$begingroup$


I have the relations



$$r_0^pm = frac12left (frachat rho_0zeta_1^1/2hat rho_1zeta_0^1/2 pm fraczeta_0^1/2zeta_1^1/2 right )$$



$$r_1^pm = frac12left (frachat rho_1zeta_2^1/2hat rho_2zeta_1^1/2 pm fraczeta_1^1/2zeta_2^1/2right )$$



$$T_0,1 = frac1r_0,1^+$$
$$R_0,1= -fracr_0,1^-r_0,1^+$$



and I'm trying to show that



$$R_0,1^2+T_0,1^2 = 1.$$



if $hat rho_0 = hat rho_2$ and $zeta_0=zeta_2.$



So far I've failed to show this. When I compute the above, I get



$$R_0^2+T_0^2 = frachat rho_1^2 zeta_0^2 + 4hat rho_1^2 zeta_0 zeta_1 - 2 hat rho_1 hat rho_0 zeta_0 zeta_1 + hat rho_0^2 zeta_1^2(hat rho_1 zeta_0 + hat rho_0 zeta_1)^2$$



If I could somehow find a way to factor this to achieve $1$, it would be great. Could anyone cast an eye over this to see if I'm not spotting the obvious?



Thanks in advance.










share|cite|improve this question









$endgroup$











  • $begingroup$
    What are $r_0,1^+$ and $r_0,1^-$?
    $endgroup$
    – someguy
    yesterday











  • $begingroup$
    They are linking terms for waves moving through a medium
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I'm asking how they relate to the first two equations.
    $endgroup$
    – someguy
    yesterday










  • $begingroup$
    I don't understand your question. $T_0,1$ and $R_0,1$ depend on the $r$ expressions.
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I see what might be different notations, e.g. $r_0^+$, $r_1^+$ and $r_0,1^+$. Is the latter the product of the first two?
    $endgroup$
    – someguy
    yesterday
















1












$begingroup$


I have the relations



$$r_0^pm = frac12left (frachat rho_0zeta_1^1/2hat rho_1zeta_0^1/2 pm fraczeta_0^1/2zeta_1^1/2 right )$$



$$r_1^pm = frac12left (frachat rho_1zeta_2^1/2hat rho_2zeta_1^1/2 pm fraczeta_1^1/2zeta_2^1/2right )$$



$$T_0,1 = frac1r_0,1^+$$
$$R_0,1= -fracr_0,1^-r_0,1^+$$



and I'm trying to show that



$$R_0,1^2+T_0,1^2 = 1.$$



if $hat rho_0 = hat rho_2$ and $zeta_0=zeta_2.$



So far I've failed to show this. When I compute the above, I get



$$R_0^2+T_0^2 = frachat rho_1^2 zeta_0^2 + 4hat rho_1^2 zeta_0 zeta_1 - 2 hat rho_1 hat rho_0 zeta_0 zeta_1 + hat rho_0^2 zeta_1^2(hat rho_1 zeta_0 + hat rho_0 zeta_1)^2$$



If I could somehow find a way to factor this to achieve $1$, it would be great. Could anyone cast an eye over this to see if I'm not spotting the obvious?



Thanks in advance.










share|cite|improve this question









$endgroup$











  • $begingroup$
    What are $r_0,1^+$ and $r_0,1^-$?
    $endgroup$
    – someguy
    yesterday











  • $begingroup$
    They are linking terms for waves moving through a medium
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I'm asking how they relate to the first two equations.
    $endgroup$
    – someguy
    yesterday










  • $begingroup$
    I don't understand your question. $T_0,1$ and $R_0,1$ depend on the $r$ expressions.
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I see what might be different notations, e.g. $r_0^+$, $r_1^+$ and $r_0,1^+$. Is the latter the product of the first two?
    $endgroup$
    – someguy
    yesterday














1












1








1





$begingroup$


I have the relations



$$r_0^pm = frac12left (frachat rho_0zeta_1^1/2hat rho_1zeta_0^1/2 pm fraczeta_0^1/2zeta_1^1/2 right )$$



$$r_1^pm = frac12left (frachat rho_1zeta_2^1/2hat rho_2zeta_1^1/2 pm fraczeta_1^1/2zeta_2^1/2right )$$



$$T_0,1 = frac1r_0,1^+$$
$$R_0,1= -fracr_0,1^-r_0,1^+$$



and I'm trying to show that



$$R_0,1^2+T_0,1^2 = 1.$$



if $hat rho_0 = hat rho_2$ and $zeta_0=zeta_2.$



So far I've failed to show this. When I compute the above, I get



$$R_0^2+T_0^2 = frachat rho_1^2 zeta_0^2 + 4hat rho_1^2 zeta_0 zeta_1 - 2 hat rho_1 hat rho_0 zeta_0 zeta_1 + hat rho_0^2 zeta_1^2(hat rho_1 zeta_0 + hat rho_0 zeta_1)^2$$



If I could somehow find a way to factor this to achieve $1$, it would be great. Could anyone cast an eye over this to see if I'm not spotting the obvious?



Thanks in advance.










share|cite|improve this question









$endgroup$




I have the relations



$$r_0^pm = frac12left (frachat rho_0zeta_1^1/2hat rho_1zeta_0^1/2 pm fraczeta_0^1/2zeta_1^1/2 right )$$



$$r_1^pm = frac12left (frachat rho_1zeta_2^1/2hat rho_2zeta_1^1/2 pm fraczeta_1^1/2zeta_2^1/2right )$$



$$T_0,1 = frac1r_0,1^+$$
$$R_0,1= -fracr_0,1^-r_0,1^+$$



and I'm trying to show that



$$R_0,1^2+T_0,1^2 = 1.$$



if $hat rho_0 = hat rho_2$ and $zeta_0=zeta_2.$



So far I've failed to show this. When I compute the above, I get



$$R_0^2+T_0^2 = frachat rho_1^2 zeta_0^2 + 4hat rho_1^2 zeta_0 zeta_1 - 2 hat rho_1 hat rho_0 zeta_0 zeta_1 + hat rho_0^2 zeta_1^2(hat rho_1 zeta_0 + hat rho_0 zeta_1)^2$$



If I could somehow find a way to factor this to achieve $1$, it would be great. Could anyone cast an eye over this to see if I'm not spotting the obvious?



Thanks in advance.







algebra-precalculus






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked yesterday









rodger_kicksrodger_kicks

8110




8110











  • $begingroup$
    What are $r_0,1^+$ and $r_0,1^-$?
    $endgroup$
    – someguy
    yesterday











  • $begingroup$
    They are linking terms for waves moving through a medium
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I'm asking how they relate to the first two equations.
    $endgroup$
    – someguy
    yesterday










  • $begingroup$
    I don't understand your question. $T_0,1$ and $R_0,1$ depend on the $r$ expressions.
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I see what might be different notations, e.g. $r_0^+$, $r_1^+$ and $r_0,1^+$. Is the latter the product of the first two?
    $endgroup$
    – someguy
    yesterday

















  • $begingroup$
    What are $r_0,1^+$ and $r_0,1^-$?
    $endgroup$
    – someguy
    yesterday











  • $begingroup$
    They are linking terms for waves moving through a medium
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I'm asking how they relate to the first two equations.
    $endgroup$
    – someguy
    yesterday










  • $begingroup$
    I don't understand your question. $T_0,1$ and $R_0,1$ depend on the $r$ expressions.
    $endgroup$
    – rodger_kicks
    yesterday










  • $begingroup$
    I see what might be different notations, e.g. $r_0^+$, $r_1^+$ and $r_0,1^+$. Is the latter the product of the first two?
    $endgroup$
    – someguy
    yesterday
















$begingroup$
What are $r_0,1^+$ and $r_0,1^-$?
$endgroup$
– someguy
yesterday





$begingroup$
What are $r_0,1^+$ and $r_0,1^-$?
$endgroup$
– someguy
yesterday













$begingroup$
They are linking terms for waves moving through a medium
$endgroup$
– rodger_kicks
yesterday




$begingroup$
They are linking terms for waves moving through a medium
$endgroup$
– rodger_kicks
yesterday












$begingroup$
I'm asking how they relate to the first two equations.
$endgroup$
– someguy
yesterday




$begingroup$
I'm asking how they relate to the first two equations.
$endgroup$
– someguy
yesterday












$begingroup$
I don't understand your question. $T_0,1$ and $R_0,1$ depend on the $r$ expressions.
$endgroup$
– rodger_kicks
yesterday




$begingroup$
I don't understand your question. $T_0,1$ and $R_0,1$ depend on the $r$ expressions.
$endgroup$
– rodger_kicks
yesterday












$begingroup$
I see what might be different notations, e.g. $r_0^+$, $r_1^+$ and $r_0,1^+$. Is the latter the product of the first two?
$endgroup$
– someguy
yesterday





$begingroup$
I see what might be different notations, e.g. $r_0^+$, $r_1^+$ and $r_0,1^+$. Is the latter the product of the first two?
$endgroup$
– someguy
yesterday











1 Answer
1






active

oldest

votes


















0












$begingroup$

For $iin0,1$ you want to show that $R_i^2+T_i^2=1$, or equivalently
$$(r_i^+)^2-(r_i^-)^2=1.$$
For the sake of legibility let $a_k:=hatrho_k$ and $b_k:=zeta_k^1/2$. Then for $i=0$ we have
$$r_0^pm=frac12left(fraca_0b_1a_1b_0pm fracb_0b_1right)
=fraca_0b_1^2pm a_1b_0^22a_1b_0b_1,$$

and so the standard identity $(x+y)^2-(x-y)^2=4xy$ shows that
begineqnarray*
(r_0^+)^2-(r_0^-)^2
&=&frac(a_0b_1^2+a_1b_0^2)^24a_1^2b_0^2b_1^2
-frac(a_0b_1^2-a_1b_0^2)^24a_1^2b_0^2b_1^2\
&=&4fraca_0a_1b_0^2b_1^24a_1^2b_0^2b_1^2=fraca_0a_1,
endeqnarray*

and so the identity holds if and only if $a_0=a_1$. Because $a_2=a_0$ and $b_2=b_0$, the exact same proof works for $i=1$ by changing the indices; change all the $0$'s to $1$'s and all the $1$'s to $0$'s.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
    $endgroup$
    – rodger_kicks
    16 hours ago











  • $begingroup$
    I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
    $endgroup$
    – rodger_kicks
    15 hours ago











  • $begingroup$
    @rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
    $endgroup$
    – Servaes
    15 hours ago











Your Answer





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1 Answer
1






active

oldest

votes








1 Answer
1






active

oldest

votes









active

oldest

votes






active

oldest

votes









0












$begingroup$

For $iin0,1$ you want to show that $R_i^2+T_i^2=1$, or equivalently
$$(r_i^+)^2-(r_i^-)^2=1.$$
For the sake of legibility let $a_k:=hatrho_k$ and $b_k:=zeta_k^1/2$. Then for $i=0$ we have
$$r_0^pm=frac12left(fraca_0b_1a_1b_0pm fracb_0b_1right)
=fraca_0b_1^2pm a_1b_0^22a_1b_0b_1,$$

and so the standard identity $(x+y)^2-(x-y)^2=4xy$ shows that
begineqnarray*
(r_0^+)^2-(r_0^-)^2
&=&frac(a_0b_1^2+a_1b_0^2)^24a_1^2b_0^2b_1^2
-frac(a_0b_1^2-a_1b_0^2)^24a_1^2b_0^2b_1^2\
&=&4fraca_0a_1b_0^2b_1^24a_1^2b_0^2b_1^2=fraca_0a_1,
endeqnarray*

and so the identity holds if and only if $a_0=a_1$. Because $a_2=a_0$ and $b_2=b_0$, the exact same proof works for $i=1$ by changing the indices; change all the $0$'s to $1$'s and all the $1$'s to $0$'s.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
    $endgroup$
    – rodger_kicks
    16 hours ago











  • $begingroup$
    I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
    $endgroup$
    – rodger_kicks
    15 hours ago











  • $begingroup$
    @rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
    $endgroup$
    – Servaes
    15 hours ago
















0












$begingroup$

For $iin0,1$ you want to show that $R_i^2+T_i^2=1$, or equivalently
$$(r_i^+)^2-(r_i^-)^2=1.$$
For the sake of legibility let $a_k:=hatrho_k$ and $b_k:=zeta_k^1/2$. Then for $i=0$ we have
$$r_0^pm=frac12left(fraca_0b_1a_1b_0pm fracb_0b_1right)
=fraca_0b_1^2pm a_1b_0^22a_1b_0b_1,$$

and so the standard identity $(x+y)^2-(x-y)^2=4xy$ shows that
begineqnarray*
(r_0^+)^2-(r_0^-)^2
&=&frac(a_0b_1^2+a_1b_0^2)^24a_1^2b_0^2b_1^2
-frac(a_0b_1^2-a_1b_0^2)^24a_1^2b_0^2b_1^2\
&=&4fraca_0a_1b_0^2b_1^24a_1^2b_0^2b_1^2=fraca_0a_1,
endeqnarray*

and so the identity holds if and only if $a_0=a_1$. Because $a_2=a_0$ and $b_2=b_0$, the exact same proof works for $i=1$ by changing the indices; change all the $0$'s to $1$'s and all the $1$'s to $0$'s.






share|cite|improve this answer











$endgroup$












  • $begingroup$
    Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
    $endgroup$
    – rodger_kicks
    16 hours ago











  • $begingroup$
    I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
    $endgroup$
    – rodger_kicks
    15 hours ago











  • $begingroup$
    @rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
    $endgroup$
    – Servaes
    15 hours ago














0












0








0





$begingroup$

For $iin0,1$ you want to show that $R_i^2+T_i^2=1$, or equivalently
$$(r_i^+)^2-(r_i^-)^2=1.$$
For the sake of legibility let $a_k:=hatrho_k$ and $b_k:=zeta_k^1/2$. Then for $i=0$ we have
$$r_0^pm=frac12left(fraca_0b_1a_1b_0pm fracb_0b_1right)
=fraca_0b_1^2pm a_1b_0^22a_1b_0b_1,$$

and so the standard identity $(x+y)^2-(x-y)^2=4xy$ shows that
begineqnarray*
(r_0^+)^2-(r_0^-)^2
&=&frac(a_0b_1^2+a_1b_0^2)^24a_1^2b_0^2b_1^2
-frac(a_0b_1^2-a_1b_0^2)^24a_1^2b_0^2b_1^2\
&=&4fraca_0a_1b_0^2b_1^24a_1^2b_0^2b_1^2=fraca_0a_1,
endeqnarray*

and so the identity holds if and only if $a_0=a_1$. Because $a_2=a_0$ and $b_2=b_0$, the exact same proof works for $i=1$ by changing the indices; change all the $0$'s to $1$'s and all the $1$'s to $0$'s.






share|cite|improve this answer











$endgroup$



For $iin0,1$ you want to show that $R_i^2+T_i^2=1$, or equivalently
$$(r_i^+)^2-(r_i^-)^2=1.$$
For the sake of legibility let $a_k:=hatrho_k$ and $b_k:=zeta_k^1/2$. Then for $i=0$ we have
$$r_0^pm=frac12left(fraca_0b_1a_1b_0pm fracb_0b_1right)
=fraca_0b_1^2pm a_1b_0^22a_1b_0b_1,$$

and so the standard identity $(x+y)^2-(x-y)^2=4xy$ shows that
begineqnarray*
(r_0^+)^2-(r_0^-)^2
&=&frac(a_0b_1^2+a_1b_0^2)^24a_1^2b_0^2b_1^2
-frac(a_0b_1^2-a_1b_0^2)^24a_1^2b_0^2b_1^2\
&=&4fraca_0a_1b_0^2b_1^24a_1^2b_0^2b_1^2=fraca_0a_1,
endeqnarray*

and so the identity holds if and only if $a_0=a_1$. Because $a_2=a_0$ and $b_2=b_0$, the exact same proof works for $i=1$ by changing the indices; change all the $0$'s to $1$'s and all the $1$'s to $0$'s.







share|cite|improve this answer














share|cite|improve this answer



share|cite|improve this answer








edited 15 hours ago

























answered yesterday









ServaesServaes

27.5k34098




27.5k34098











  • $begingroup$
    Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
    $endgroup$
    – rodger_kicks
    16 hours ago











  • $begingroup$
    I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
    $endgroup$
    – rodger_kicks
    15 hours ago











  • $begingroup$
    @rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
    $endgroup$
    – Servaes
    15 hours ago

















  • $begingroup$
    Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
    $endgroup$
    – rodger_kicks
    16 hours ago











  • $begingroup$
    I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
    $endgroup$
    – rodger_kicks
    15 hours ago











  • $begingroup$
    @rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
    $endgroup$
    – Servaes
    15 hours ago
















$begingroup$
Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
$endgroup$
– rodger_kicks
16 hours ago





$begingroup$
Hi, I think you have a made a mistake, on the second terms in the last line. For this to hold we would need $4a_0a_1b_0^2 b_1^2$ on the numerator? So this only holds if $a_0=a_1$
$endgroup$
– rodger_kicks
16 hours ago













$begingroup$
I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
$endgroup$
– rodger_kicks
15 hours ago





$begingroup$
I was thinking of some way to achieve the relation purely in terms of $a_0,2,b_0,2$ so that I can then apply $a_2=a_0, b_0=b_2.$ The problem arises with the $a_1,b_1$ terms...
$endgroup$
– rodger_kicks
15 hours ago













$begingroup$
@rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
$endgroup$
– Servaes
15 hours ago





$begingroup$
@rodger_kicks You are absolutely right, I have adjusted my answer accordingly. I don't understand what you mean by your second comment.
$endgroup$
– Servaes
15 hours ago


















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