Confusion regarding Fourier half series for sine and cosine The 2019 Stack Overflow Developer Survey Results Are InRelation between “harmonic form” and fourier series?Fourier cosine series and sum helpWhat is a fast method for evaluate this trigonometric series?Fourier series with half rangeFourier Cosine Series questionFourier cosine series giving nonsense answerFourier Series. Relevance of the period of sine and cosineUndefined term in Fourier seriesFourier Series Expansion for Half-Wave Sine ProblemComplex sum of sine and cosine function
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Confusion regarding Fourier half series for sine and cosine
The 2019 Stack Overflow Developer Survey Results Are InRelation between “harmonic form” and fourier series?Fourier cosine series and sum helpWhat is a fast method for evaluate this trigonometric series?Fourier series with half rangeFourier Cosine Series questionFourier cosine series giving nonsense answerFourier Series. Relevance of the period of sine and cosineUndefined term in Fourier seriesFourier Series Expansion for Half-Wave Sine ProblemComplex sum of sine and cosine function
$begingroup$
I have been struggling with a problem for a long time. Solving a second order partial differential equation using Fourier half series in sine with the help of Mathematica gives me
$$
phi_mine(x,y)=-sum_k=1,3,5,...^inftyfrac8 a^2 G_zy theta left(textsechleft(fracpi b k2 a fracsqrtG_zxsqrtG_zy right) cosh left(fracpi k ya fracsqrtG_zxsqrtG_zyright)-1right)pi ^3 k^3sin left(fracpi k xaright)
$$
where $G_zy$, $G_zx$, $theta$, $a$, and $b$ are constants.
This is almost exactly what is written in the solution that I have, which is
$$
phi_sol(x,y)=frac8pi^3 G_zy a^2 sum_k=1,3,5,...^inftyfrac(-1)^(k-1)/2k^3left( 1-fraccosh left(fracpi k mu ayright)cosh left(fracb pi k mu2 aright) right)cos left(fracpi kaxright)
$$
where $mu=sqrtfracG_zxG_zy$.
$phi_sol(x,y)$ is missing $theta$ but I suspect that it's a typo. I've been trying to figure out the difference between my answer and the solution and all I can find is that somehow
$$
sin left(fracpi k xaright)=cosleft(fracpi k xaright) (-1)^(k-1)/2
$$
for $k=1,3,5,...$ I've never seen this and when I plot them they give different curves so they don't seem to be equivalent.
As can be seen, $a$ determines the amplitude of the periodic functions so that $
sin left(fracpi k xaright)$ is always $0$ at -1 and 1. $cosleft(fracpi k xaright) (-1)^(k-1)/2$ on the other hand flips from $1$ to $-1$ at $pm a$.
The next step in the process involves working out the constant $beta$,
$$
beta=frac2 int_0^b left(int_0^a phi (x,y) , dxright) , dyG_zx a b^3
$$
I get that $phi_sol(x,y)$ converges to a value while $phi_mine(x,y)$ goes to infinity. Therefore I'm doing something wrong but I'm not sure what. Is it possible to change $sin left(fracpi k xaright)$ into $cosleft(fracpi k xaright) (-1)^(k-1)/2$?
fourier-series trigonometric-series
$endgroup$
add a comment |
$begingroup$
I have been struggling with a problem for a long time. Solving a second order partial differential equation using Fourier half series in sine with the help of Mathematica gives me
$$
phi_mine(x,y)=-sum_k=1,3,5,...^inftyfrac8 a^2 G_zy theta left(textsechleft(fracpi b k2 a fracsqrtG_zxsqrtG_zy right) cosh left(fracpi k ya fracsqrtG_zxsqrtG_zyright)-1right)pi ^3 k^3sin left(fracpi k xaright)
$$
where $G_zy$, $G_zx$, $theta$, $a$, and $b$ are constants.
This is almost exactly what is written in the solution that I have, which is
$$
phi_sol(x,y)=frac8pi^3 G_zy a^2 sum_k=1,3,5,...^inftyfrac(-1)^(k-1)/2k^3left( 1-fraccosh left(fracpi k mu ayright)cosh left(fracb pi k mu2 aright) right)cos left(fracpi kaxright)
$$
where $mu=sqrtfracG_zxG_zy$.
$phi_sol(x,y)$ is missing $theta$ but I suspect that it's a typo. I've been trying to figure out the difference between my answer and the solution and all I can find is that somehow
$$
sin left(fracpi k xaright)=cosleft(fracpi k xaright) (-1)^(k-1)/2
$$
for $k=1,3,5,...$ I've never seen this and when I plot them they give different curves so they don't seem to be equivalent.
As can be seen, $a$ determines the amplitude of the periodic functions so that $
sin left(fracpi k xaright)$ is always $0$ at -1 and 1. $cosleft(fracpi k xaright) (-1)^(k-1)/2$ on the other hand flips from $1$ to $-1$ at $pm a$.
The next step in the process involves working out the constant $beta$,
$$
beta=frac2 int_0^b left(int_0^a phi (x,y) , dxright) , dyG_zx a b^3
$$
I get that $phi_sol(x,y)$ converges to a value while $phi_mine(x,y)$ goes to infinity. Therefore I'm doing something wrong but I'm not sure what. Is it possible to change $sin left(fracpi k xaright)$ into $cosleft(fracpi k xaright) (-1)^(k-1)/2$?
fourier-series trigonometric-series
$endgroup$
$begingroup$
No, that's wrong. I corrected it, thanks for pointing it out.
$endgroup$
– enea19
Apr 8 at 1:07
add a comment |
$begingroup$
I have been struggling with a problem for a long time. Solving a second order partial differential equation using Fourier half series in sine with the help of Mathematica gives me
$$
phi_mine(x,y)=-sum_k=1,3,5,...^inftyfrac8 a^2 G_zy theta left(textsechleft(fracpi b k2 a fracsqrtG_zxsqrtG_zy right) cosh left(fracpi k ya fracsqrtG_zxsqrtG_zyright)-1right)pi ^3 k^3sin left(fracpi k xaright)
$$
where $G_zy$, $G_zx$, $theta$, $a$, and $b$ are constants.
This is almost exactly what is written in the solution that I have, which is
$$
phi_sol(x,y)=frac8pi^3 G_zy a^2 sum_k=1,3,5,...^inftyfrac(-1)^(k-1)/2k^3left( 1-fraccosh left(fracpi k mu ayright)cosh left(fracb pi k mu2 aright) right)cos left(fracpi kaxright)
$$
where $mu=sqrtfracG_zxG_zy$.
$phi_sol(x,y)$ is missing $theta$ but I suspect that it's a typo. I've been trying to figure out the difference between my answer and the solution and all I can find is that somehow
$$
sin left(fracpi k xaright)=cosleft(fracpi k xaright) (-1)^(k-1)/2
$$
for $k=1,3,5,...$ I've never seen this and when I plot them they give different curves so they don't seem to be equivalent.
As can be seen, $a$ determines the amplitude of the periodic functions so that $
sin left(fracpi k xaright)$ is always $0$ at -1 and 1. $cosleft(fracpi k xaright) (-1)^(k-1)/2$ on the other hand flips from $1$ to $-1$ at $pm a$.
The next step in the process involves working out the constant $beta$,
$$
beta=frac2 int_0^b left(int_0^a phi (x,y) , dxright) , dyG_zx a b^3
$$
I get that $phi_sol(x,y)$ converges to a value while $phi_mine(x,y)$ goes to infinity. Therefore I'm doing something wrong but I'm not sure what. Is it possible to change $sin left(fracpi k xaright)$ into $cosleft(fracpi k xaright) (-1)^(k-1)/2$?
fourier-series trigonometric-series
$endgroup$
I have been struggling with a problem for a long time. Solving a second order partial differential equation using Fourier half series in sine with the help of Mathematica gives me
$$
phi_mine(x,y)=-sum_k=1,3,5,...^inftyfrac8 a^2 G_zy theta left(textsechleft(fracpi b k2 a fracsqrtG_zxsqrtG_zy right) cosh left(fracpi k ya fracsqrtG_zxsqrtG_zyright)-1right)pi ^3 k^3sin left(fracpi k xaright)
$$
where $G_zy$, $G_zx$, $theta$, $a$, and $b$ are constants.
This is almost exactly what is written in the solution that I have, which is
$$
phi_sol(x,y)=frac8pi^3 G_zy a^2 sum_k=1,3,5,...^inftyfrac(-1)^(k-1)/2k^3left( 1-fraccosh left(fracpi k mu ayright)cosh left(fracb pi k mu2 aright) right)cos left(fracpi kaxright)
$$
where $mu=sqrtfracG_zxG_zy$.
$phi_sol(x,y)$ is missing $theta$ but I suspect that it's a typo. I've been trying to figure out the difference between my answer and the solution and all I can find is that somehow
$$
sin left(fracpi k xaright)=cosleft(fracpi k xaright) (-1)^(k-1)/2
$$
for $k=1,3,5,...$ I've never seen this and when I plot them they give different curves so they don't seem to be equivalent.
As can be seen, $a$ determines the amplitude of the periodic functions so that $
sin left(fracpi k xaright)$ is always $0$ at -1 and 1. $cosleft(fracpi k xaright) (-1)^(k-1)/2$ on the other hand flips from $1$ to $-1$ at $pm a$.
The next step in the process involves working out the constant $beta$,
$$
beta=frac2 int_0^b left(int_0^a phi (x,y) , dxright) , dyG_zx a b^3
$$
I get that $phi_sol(x,y)$ converges to a value while $phi_mine(x,y)$ goes to infinity. Therefore I'm doing something wrong but I'm not sure what. Is it possible to change $sin left(fracpi k xaright)$ into $cosleft(fracpi k xaright) (-1)^(k-1)/2$?
fourier-series trigonometric-series
fourier-series trigonometric-series
edited Apr 8 at 1:07
enea19
asked Apr 7 at 10:52
enea19enea19
374
374
$begingroup$
No, that's wrong. I corrected it, thanks for pointing it out.
$endgroup$
– enea19
Apr 8 at 1:07
add a comment |
$begingroup$
No, that's wrong. I corrected it, thanks for pointing it out.
$endgroup$
– enea19
Apr 8 at 1:07
$begingroup$
No, that's wrong. I corrected it, thanks for pointing it out.
$endgroup$
– enea19
Apr 8 at 1:07
$begingroup$
No, that's wrong. I corrected it, thanks for pointing it out.
$endgroup$
– enea19
Apr 8 at 1:07
add a comment |
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$begingroup$
No, that's wrong. I corrected it, thanks for pointing it out.
$endgroup$
– enea19
Apr 8 at 1:07