Solve initial value problem $u_t+x^2u_x=0$ by method of characteristics
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Related Question:
- Using method of characteristics to solve transport equation
Solve the initial value problem using the method of characteristics
$$u_t+x^2u_x=0 ~~~~-infty<x<infty,~~~ t> 0$$
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Here is what I have done so far.
We are given that $u_t+x^2u_x=0$. Therefore, we know that this is a type of transport equation in which we can write the general form as $A(x,t)u_t+B(x,t)u_x=0$. Hence, we have
$$frac{dt}{A}=frac{dx}{B}$$
as our characteristic equations. In our example,
$$frac{dt}{1}=frac{dx}{x^2}$$
So,
$$ frac{dx}{x^2}=dt~~Rightarrow~~~ -frac{1}{x} = t+C ~~Rightarrow~~~ C=-t-frac{1}{x}$$
Therefore, $u(x,t)$ is constant along the curves where $C=-t-frac{1}{x}$. Thus, the general solution is
$$u(x,t)=fBig(-t-frac{1}{x}Big)$$
where f is an arbitrary differentiable function. We now need to apply our initial data. We are given that
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Therefore,
$$u(x,0)=fBig(-frac{1}{x}Big)=left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
However, I'm not sure what to do with the piecewise-defined initial conditions after this step. We would have $f(-frac{1}{x})=0$ or $f(-frac{1}{x})=1$ which would indicate that f is a constant function.
pde
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add a comment |
$begingroup$
Related Question:
- Using method of characteristics to solve transport equation
Solve the initial value problem using the method of characteristics
$$u_t+x^2u_x=0 ~~~~-infty<x<infty,~~~ t> 0$$
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Here is what I have done so far.
We are given that $u_t+x^2u_x=0$. Therefore, we know that this is a type of transport equation in which we can write the general form as $A(x,t)u_t+B(x,t)u_x=0$. Hence, we have
$$frac{dt}{A}=frac{dx}{B}$$
as our characteristic equations. In our example,
$$frac{dt}{1}=frac{dx}{x^2}$$
So,
$$ frac{dx}{x^2}=dt~~Rightarrow~~~ -frac{1}{x} = t+C ~~Rightarrow~~~ C=-t-frac{1}{x}$$
Therefore, $u(x,t)$ is constant along the curves where $C=-t-frac{1}{x}$. Thus, the general solution is
$$u(x,t)=fBig(-t-frac{1}{x}Big)$$
where f is an arbitrary differentiable function. We now need to apply our initial data. We are given that
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Therefore,
$$u(x,0)=fBig(-frac{1}{x}Big)=left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
However, I'm not sure what to do with the piecewise-defined initial conditions after this step. We would have $f(-frac{1}{x})=0$ or $f(-frac{1}{x})=1$ which would indicate that f is a constant function.
pde
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$begingroup$
You have a shock forming due to your initial condition. You'll need to do a fair bit more work to get the solution. There are plenty of problems on the site providing a step by step solution on how to solve these types of problems.
$endgroup$
– Mattos
Jan 14 at 5:08
add a comment |
$begingroup$
Related Question:
- Using method of characteristics to solve transport equation
Solve the initial value problem using the method of characteristics
$$u_t+x^2u_x=0 ~~~~-infty<x<infty,~~~ t> 0$$
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Here is what I have done so far.
We are given that $u_t+x^2u_x=0$. Therefore, we know that this is a type of transport equation in which we can write the general form as $A(x,t)u_t+B(x,t)u_x=0$. Hence, we have
$$frac{dt}{A}=frac{dx}{B}$$
as our characteristic equations. In our example,
$$frac{dt}{1}=frac{dx}{x^2}$$
So,
$$ frac{dx}{x^2}=dt~~Rightarrow~~~ -frac{1}{x} = t+C ~~Rightarrow~~~ C=-t-frac{1}{x}$$
Therefore, $u(x,t)$ is constant along the curves where $C=-t-frac{1}{x}$. Thus, the general solution is
$$u(x,t)=fBig(-t-frac{1}{x}Big)$$
where f is an arbitrary differentiable function. We now need to apply our initial data. We are given that
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Therefore,
$$u(x,0)=fBig(-frac{1}{x}Big)=left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
However, I'm not sure what to do with the piecewise-defined initial conditions after this step. We would have $f(-frac{1}{x})=0$ or $f(-frac{1}{x})=1$ which would indicate that f is a constant function.
pde
$endgroup$
Related Question:
- Using method of characteristics to solve transport equation
Solve the initial value problem using the method of characteristics
$$u_t+x^2u_x=0 ~~~~-infty<x<infty,~~~ t> 0$$
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Here is what I have done so far.
We are given that $u_t+x^2u_x=0$. Therefore, we know that this is a type of transport equation in which we can write the general form as $A(x,t)u_t+B(x,t)u_x=0$. Hence, we have
$$frac{dt}{A}=frac{dx}{B}$$
as our characteristic equations. In our example,
$$frac{dt}{1}=frac{dx}{x^2}$$
So,
$$ frac{dx}{x^2}=dt~~Rightarrow~~~ -frac{1}{x} = t+C ~~Rightarrow~~~ C=-t-frac{1}{x}$$
Therefore, $u(x,t)$ is constant along the curves where $C=-t-frac{1}{x}$. Thus, the general solution is
$$u(x,t)=fBig(-t-frac{1}{x}Big)$$
where f is an arbitrary differentiable function. We now need to apply our initial data. We are given that
$$
u(x,0) = left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
Therefore,
$$u(x,0)=fBig(-frac{1}{x}Big)=left{
begin{array}{ll}
1, & quad 0leq x leq 1 \
0, & quad otherwise
end{array}
right.
$$
However, I'm not sure what to do with the piecewise-defined initial conditions after this step. We would have $f(-frac{1}{x})=0$ or $f(-frac{1}{x})=1$ which would indicate that f is a constant function.
pde
pde
asked Jan 13 at 18:20
Axion004Axion004
374313
374313
$begingroup$
You have a shock forming due to your initial condition. You'll need to do a fair bit more work to get the solution. There are plenty of problems on the site providing a step by step solution on how to solve these types of problems.
$endgroup$
– Mattos
Jan 14 at 5:08
add a comment |
$begingroup$
You have a shock forming due to your initial condition. You'll need to do a fair bit more work to get the solution. There are plenty of problems on the site providing a step by step solution on how to solve these types of problems.
$endgroup$
– Mattos
Jan 14 at 5:08
$begingroup$
You have a shock forming due to your initial condition. You'll need to do a fair bit more work to get the solution. There are plenty of problems on the site providing a step by step solution on how to solve these types of problems.
$endgroup$
– Mattos
Jan 14 at 5:08
$begingroup$
You have a shock forming due to your initial condition. You'll need to do a fair bit more work to get the solution. There are plenty of problems on the site providing a step by step solution on how to solve these types of problems.
$endgroup$
– Mattos
Jan 14 at 5:08
add a comment |
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$begingroup$
You have a shock forming due to your initial condition. You'll need to do a fair bit more work to get the solution. There are plenty of problems on the site providing a step by step solution on how to solve these types of problems.
$endgroup$
– Mattos
Jan 14 at 5:08