Solve initial value problem $u_t+x^2u_x=0$ by method of characteristics












0












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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.










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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


















0












$begingroup$


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.










share|cite|improve this question









$endgroup$












  • $begingroup$
    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
















0












0








0





$begingroup$


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.










share|cite|improve this question









$endgroup$




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






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asked Jan 13 at 18:20









Axion004Axion004

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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




















  • $begingroup$
    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












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