Question about the Dirac-delta function The 2019 Stack Overflow Developer Survey Results Are InDiffusion equation in an infinite mediumDirac Delta Function as Initial condition for 1D Diffusion PDE: ONE or TWO equations(conditions)?Solving Poisson's equation for $varrho(mathbfr) = sigma cosleft(frac2 piL xright) , delta(y)$Inverse fourier transform for the heat equationA specific partial differential equation using Fourier TransformFourier Transform Dirac DeltaUsing the Dirac Delta function in PDE'sRepresentation formula for harmonic function and Dirac Delta functionPartial Differential Equation using Fourier Sine TransformQuestions about the heat equation
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Question about the Dirac-delta function
The 2019 Stack Overflow Developer Survey Results Are InDiffusion equation in an infinite mediumDirac Delta Function as Initial condition for 1D Diffusion PDE: ONE or TWO equations(conditions)?Solving Poisson's equation for $varrho(mathbfr) = sigma cosleft(frac2 piL xright) , delta(y)$Inverse fourier transform for the heat equationA specific partial differential equation using Fourier TransformFourier Transform Dirac DeltaUsing the Dirac Delta function in PDE'sRepresentation formula for harmonic function and Dirac Delta functionPartial Differential Equation using Fourier Sine TransformQuestions about the heat equation
$begingroup$
The equation$$ u_t = frac14 u_xx, ; ; ; (x,t) in Omega = (- infty,
infty) times (0, infty) $$
can be solved using Fourier transform and the solution is
$$ u(x,t) = frac1sqrt pi t intlimits_-infty^infty
g(y) mathrme^ - (x-y)^2/ t mathrmd y $$
What is the solution for initial condition $u(x,0) = delta(x+1)$?
Where $delta(x)$ is the Dirac delta function
thought:
We know $g(x) = u(x,0)$ is the initial condition. I know $delta(x+1) = infty$ when $x=-1$ and zero otherwise. So, if I plug this into my solution I get something of the form
$$ u(x,t) = frac1sqrtpi t * (infty ) * mathrme^ - (x+1)^2/ t $$
How to simplify such expression?
pde
$endgroup$
add a comment |
$begingroup$
The equation$$ u_t = frac14 u_xx, ; ; ; (x,t) in Omega = (- infty,
infty) times (0, infty) $$
can be solved using Fourier transform and the solution is
$$ u(x,t) = frac1sqrt pi t intlimits_-infty^infty
g(y) mathrme^ - (x-y)^2/ t mathrmd y $$
What is the solution for initial condition $u(x,0) = delta(x+1)$?
Where $delta(x)$ is the Dirac delta function
thought:
We know $g(x) = u(x,0)$ is the initial condition. I know $delta(x+1) = infty$ when $x=-1$ and zero otherwise. So, if I plug this into my solution I get something of the form
$$ u(x,t) = frac1sqrtpi t * (infty ) * mathrme^ - (x+1)^2/ t $$
How to simplify such expression?
pde
$endgroup$
1
$begingroup$
Forget the informal "$=infty$ when $x=0$ and $=0$ otherwise" description of the delta-function. The (or a) proper definition of the delta function is in how it acts under an integral, namely $int_-infty^infty f(x)delta(x-a)rm dx equiv f(a)$. This is all you need here.
$endgroup$
– Winther
Mar 23 at 19:25
add a comment |
$begingroup$
The equation$$ u_t = frac14 u_xx, ; ; ; (x,t) in Omega = (- infty,
infty) times (0, infty) $$
can be solved using Fourier transform and the solution is
$$ u(x,t) = frac1sqrt pi t intlimits_-infty^infty
g(y) mathrme^ - (x-y)^2/ t mathrmd y $$
What is the solution for initial condition $u(x,0) = delta(x+1)$?
Where $delta(x)$ is the Dirac delta function
thought:
We know $g(x) = u(x,0)$ is the initial condition. I know $delta(x+1) = infty$ when $x=-1$ and zero otherwise. So, if I plug this into my solution I get something of the form
$$ u(x,t) = frac1sqrtpi t * (infty ) * mathrme^ - (x+1)^2/ t $$
How to simplify such expression?
pde
$endgroup$
The equation$$ u_t = frac14 u_xx, ; ; ; (x,t) in Omega = (- infty,
infty) times (0, infty) $$
can be solved using Fourier transform and the solution is
$$ u(x,t) = frac1sqrt pi t intlimits_-infty^infty
g(y) mathrme^ - (x-y)^2/ t mathrmd y $$
What is the solution for initial condition $u(x,0) = delta(x+1)$?
Where $delta(x)$ is the Dirac delta function
thought:
We know $g(x) = u(x,0)$ is the initial condition. I know $delta(x+1) = infty$ when $x=-1$ and zero otherwise. So, if I plug this into my solution I get something of the form
$$ u(x,t) = frac1sqrtpi t * (infty ) * mathrme^ - (x+1)^2/ t $$
How to simplify such expression?
pde
pde
edited Mar 23 at 18:41
Bernard
124k741117
124k741117
asked Mar 23 at 18:39
JamesJames
2,636425
2,636425
1
$begingroup$
Forget the informal "$=infty$ when $x=0$ and $=0$ otherwise" description of the delta-function. The (or a) proper definition of the delta function is in how it acts under an integral, namely $int_-infty^infty f(x)delta(x-a)rm dx equiv f(a)$. This is all you need here.
$endgroup$
– Winther
Mar 23 at 19:25
add a comment |
1
$begingroup$
Forget the informal "$=infty$ when $x=0$ and $=0$ otherwise" description of the delta-function. The (or a) proper definition of the delta function is in how it acts under an integral, namely $int_-infty^infty f(x)delta(x-a)rm dx equiv f(a)$. This is all you need here.
$endgroup$
– Winther
Mar 23 at 19:25
1
1
$begingroup$
Forget the informal "$=infty$ when $x=0$ and $=0$ otherwise" description of the delta-function. The (or a) proper definition of the delta function is in how it acts under an integral, namely $int_-infty^infty f(x)delta(x-a)rm dx equiv f(a)$. This is all you need here.
$endgroup$
– Winther
Mar 23 at 19:25
$begingroup$
Forget the informal "$=infty$ when $x=0$ and $=0$ otherwise" description of the delta-function. The (or a) proper definition of the delta function is in how it acts under an integral, namely $int_-infty^infty f(x)delta(x-a)rm dx equiv f(a)$. This is all you need here.
$endgroup$
– Winther
Mar 23 at 19:25
add a comment |
1 Answer
1
active
oldest
votes
$begingroup$
In your statement, I think you mean that the function $g(y) = u(y,0)$ contains the initial conditions. Then to answer your question, you need to perform the integral with $g(y) = delta(y+1)$. This can be done quite easily since integration against a $delta$ simply evaluates the integrand at the support of the $delta$. So in your case, we would have $u(x,t) = frac1sqrtpi t e^-(x+1)^2/t$, and there is no need for the "infinity" that you write above. (Edit: I completely agree with the comment by Winther, you should probably not think of the delta function as being "equal to infinity" at the origin, just use the integral property that Winther stated as the defining property of the delta function.)
Edit to answer your comment: If we replace the $delta(x-1)$ by a Heaviside $H(x-1)$ then since
$$H(x-1) = cases0,,textfor x<1,\ 1,,textfor x>1,$$
we need to evaluate the integral
$$u(x,t)=frac1sqrtpi tint_1^inftye^-(x-y)^2/t ,mathrmdy.$$
I think you should be able to do this in terms of the error function.
$endgroup$
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
add a comment |
Your Answer
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1 Answer
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$begingroup$
In your statement, I think you mean that the function $g(y) = u(y,0)$ contains the initial conditions. Then to answer your question, you need to perform the integral with $g(y) = delta(y+1)$. This can be done quite easily since integration against a $delta$ simply evaluates the integrand at the support of the $delta$. So in your case, we would have $u(x,t) = frac1sqrtpi t e^-(x+1)^2/t$, and there is no need for the "infinity" that you write above. (Edit: I completely agree with the comment by Winther, you should probably not think of the delta function as being "equal to infinity" at the origin, just use the integral property that Winther stated as the defining property of the delta function.)
Edit to answer your comment: If we replace the $delta(x-1)$ by a Heaviside $H(x-1)$ then since
$$H(x-1) = cases0,,textfor x<1,\ 1,,textfor x>1,$$
we need to evaluate the integral
$$u(x,t)=frac1sqrtpi tint_1^inftye^-(x-y)^2/t ,mathrmdy.$$
I think you should be able to do this in terms of the error function.
$endgroup$
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
add a comment |
$begingroup$
In your statement, I think you mean that the function $g(y) = u(y,0)$ contains the initial conditions. Then to answer your question, you need to perform the integral with $g(y) = delta(y+1)$. This can be done quite easily since integration against a $delta$ simply evaluates the integrand at the support of the $delta$. So in your case, we would have $u(x,t) = frac1sqrtpi t e^-(x+1)^2/t$, and there is no need for the "infinity" that you write above. (Edit: I completely agree with the comment by Winther, you should probably not think of the delta function as being "equal to infinity" at the origin, just use the integral property that Winther stated as the defining property of the delta function.)
Edit to answer your comment: If we replace the $delta(x-1)$ by a Heaviside $H(x-1)$ then since
$$H(x-1) = cases0,,textfor x<1,\ 1,,textfor x>1,$$
we need to evaluate the integral
$$u(x,t)=frac1sqrtpi tint_1^inftye^-(x-y)^2/t ,mathrmdy.$$
I think you should be able to do this in terms of the error function.
$endgroup$
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
add a comment |
$begingroup$
In your statement, I think you mean that the function $g(y) = u(y,0)$ contains the initial conditions. Then to answer your question, you need to perform the integral with $g(y) = delta(y+1)$. This can be done quite easily since integration against a $delta$ simply evaluates the integrand at the support of the $delta$. So in your case, we would have $u(x,t) = frac1sqrtpi t e^-(x+1)^2/t$, and there is no need for the "infinity" that you write above. (Edit: I completely agree with the comment by Winther, you should probably not think of the delta function as being "equal to infinity" at the origin, just use the integral property that Winther stated as the defining property of the delta function.)
Edit to answer your comment: If we replace the $delta(x-1)$ by a Heaviside $H(x-1)$ then since
$$H(x-1) = cases0,,textfor x<1,\ 1,,textfor x>1,$$
we need to evaluate the integral
$$u(x,t)=frac1sqrtpi tint_1^inftye^-(x-y)^2/t ,mathrmdy.$$
I think you should be able to do this in terms of the error function.
$endgroup$
In your statement, I think you mean that the function $g(y) = u(y,0)$ contains the initial conditions. Then to answer your question, you need to perform the integral with $g(y) = delta(y+1)$. This can be done quite easily since integration against a $delta$ simply evaluates the integrand at the support of the $delta$. So in your case, we would have $u(x,t) = frac1sqrtpi t e^-(x+1)^2/t$, and there is no need for the "infinity" that you write above. (Edit: I completely agree with the comment by Winther, you should probably not think of the delta function as being "equal to infinity" at the origin, just use the integral property that Winther stated as the defining property of the delta function.)
Edit to answer your comment: If we replace the $delta(x-1)$ by a Heaviside $H(x-1)$ then since
$$H(x-1) = cases0,,textfor x<1,\ 1,,textfor x>1,$$
we need to evaluate the integral
$$u(x,t)=frac1sqrtpi tint_1^inftye^-(x-y)^2/t ,mathrmdy.$$
I think you should be able to do this in terms of the error function.
edited Mar 24 at 16:15
answered Mar 23 at 19:21
bobcliffebobcliffe
1506
1506
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
add a comment |
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
thanks for your asnwer. I have a question, how if we replace delta function with heaviside $H(x-1)$? How would solution look now?
$endgroup$
– James
Mar 23 at 19:28
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
$begingroup$
@JimmySabater I have added some extra comments for you :)
$endgroup$
– bobcliffe
Mar 24 at 16:16
add a comment |
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$begingroup$
Forget the informal "$=infty$ when $x=0$ and $=0$ otherwise" description of the delta-function. The (or a) proper definition of the delta function is in how it acts under an integral, namely $int_-infty^infty f(x)delta(x-a)rm dx equiv f(a)$. This is all you need here.
$endgroup$
– Winther
Mar 23 at 19:25