weak solution of linear transport (advection) equation
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How to show that $g(x-at)$ is the weak solution of the initial value problem
$$u_t+au_x=0$$
$$u(x,0)=g(x)$$ where $ g(x)in L^{infty}(mathbb{R})$
Definition: $u$ is said to be the weak solution of the above initial value problem if
$$intlimits_0 ^ {infty} intlimits_{mathbb{R}} ({u{phi}_t+au{phi}_x})dxdt =intlimits_{mathbb{R}}g(x)phi(x,0)dx$$ $forall phi in C_c ^1(mathbb{R} times[0,infty))$
pde hyperbolic-equations transport-equation
$endgroup$
add a comment |
$begingroup$
How to show that $g(x-at)$ is the weak solution of the initial value problem
$$u_t+au_x=0$$
$$u(x,0)=g(x)$$ where $ g(x)in L^{infty}(mathbb{R})$
Definition: $u$ is said to be the weak solution of the above initial value problem if
$$intlimits_0 ^ {infty} intlimits_{mathbb{R}} ({u{phi}_t+au{phi}_x})dxdt =intlimits_{mathbb{R}}g(x)phi(x,0)dx$$ $forall phi in C_c ^1(mathbb{R} times[0,infty))$
pde hyperbolic-equations transport-equation
$endgroup$
1
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You simply need to show that $u(x,t) = g(x-at)$ satisfies the integral equation for all $phiin C_c^1(mathbb{R}times [0,infty))$. Divergence theorem and integration by parts would be useful for you.
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– Chee Han
Jul 27 '18 at 22:54
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Can we apply integration by parts and divergence theorem as g is only $L^{infty}$? Could u please give the complete proof.. I am unable to follow
$endgroup$
– Rosy
Aug 3 '18 at 8:23
add a comment |
$begingroup$
How to show that $g(x-at)$ is the weak solution of the initial value problem
$$u_t+au_x=0$$
$$u(x,0)=g(x)$$ where $ g(x)in L^{infty}(mathbb{R})$
Definition: $u$ is said to be the weak solution of the above initial value problem if
$$intlimits_0 ^ {infty} intlimits_{mathbb{R}} ({u{phi}_t+au{phi}_x})dxdt =intlimits_{mathbb{R}}g(x)phi(x,0)dx$$ $forall phi in C_c ^1(mathbb{R} times[0,infty))$
pde hyperbolic-equations transport-equation
$endgroup$
How to show that $g(x-at)$ is the weak solution of the initial value problem
$$u_t+au_x=0$$
$$u(x,0)=g(x)$$ where $ g(x)in L^{infty}(mathbb{R})$
Definition: $u$ is said to be the weak solution of the above initial value problem if
$$intlimits_0 ^ {infty} intlimits_{mathbb{R}} ({u{phi}_t+au{phi}_x})dxdt =intlimits_{mathbb{R}}g(x)phi(x,0)dx$$ $forall phi in C_c ^1(mathbb{R} times[0,infty))$
pde hyperbolic-equations transport-equation
pde hyperbolic-equations transport-equation
edited Dec 6 '18 at 13:54
Harry49
6,21331132
6,21331132
asked Jul 27 '18 at 19:30
RosyRosy
1076
1076
1
$begingroup$
You simply need to show that $u(x,t) = g(x-at)$ satisfies the integral equation for all $phiin C_c^1(mathbb{R}times [0,infty))$. Divergence theorem and integration by parts would be useful for you.
$endgroup$
– Chee Han
Jul 27 '18 at 22:54
$begingroup$
Can we apply integration by parts and divergence theorem as g is only $L^{infty}$? Could u please give the complete proof.. I am unable to follow
$endgroup$
– Rosy
Aug 3 '18 at 8:23
add a comment |
1
$begingroup$
You simply need to show that $u(x,t) = g(x-at)$ satisfies the integral equation for all $phiin C_c^1(mathbb{R}times [0,infty))$. Divergence theorem and integration by parts would be useful for you.
$endgroup$
– Chee Han
Jul 27 '18 at 22:54
$begingroup$
Can we apply integration by parts and divergence theorem as g is only $L^{infty}$? Could u please give the complete proof.. I am unable to follow
$endgroup$
– Rosy
Aug 3 '18 at 8:23
1
1
$begingroup$
You simply need to show that $u(x,t) = g(x-at)$ satisfies the integral equation for all $phiin C_c^1(mathbb{R}times [0,infty))$. Divergence theorem and integration by parts would be useful for you.
$endgroup$
– Chee Han
Jul 27 '18 at 22:54
$begingroup$
You simply need to show that $u(x,t) = g(x-at)$ satisfies the integral equation for all $phiin C_c^1(mathbb{R}times [0,infty))$. Divergence theorem and integration by parts would be useful for you.
$endgroup$
– Chee Han
Jul 27 '18 at 22:54
$begingroup$
Can we apply integration by parts and divergence theorem as g is only $L^{infty}$? Could u please give the complete proof.. I am unable to follow
$endgroup$
– Rosy
Aug 3 '18 at 8:23
$begingroup$
Can we apply integration by parts and divergence theorem as g is only $L^{infty}$? Could u please give the complete proof.. I am unable to follow
$endgroup$
– Rosy
Aug 3 '18 at 8:23
add a comment |
1 Answer
1
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oldest
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$begingroup$
Let us make the change of variable $(xi, tau) = (x-at,t)$, so that $partial_t = partial_tau - apartial_xi$ and $partial_x = partial_xi$. Thus, using Fubini's theorem and integration by parts,
begin{aligned}
iint_{Bbb RtimesBbb R_+} u, (phi_t + a phi_x), text d x,text d t
&= iint_{Bbb RtimesBbb R_+} u phi_tau, text d xi,text d tau \
&= iint_{Bbb R_+timesBbb R} u phi_tau, text d tau,text d xi \
&= int_{Bbb R}left[uphiright]_{tauinBbb R_+}text dxi - iint_{Bbb R_+timesBbb R} underbrace{u_tau}_{=0} phi, text d tau,text d xi \
&= -int_{Bbb R}left.(uphi)right|_{t = 0}text dx , .
end{aligned}
We have shown that the definition holds for all smooth $phi$ with compact support. Hence, $u(x,t) = g(x-at)$ is a weak solution to the Cauchy problem of the advection equation. Note that there may be a sign mistake.
$endgroup$
add a comment |
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1 Answer
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$begingroup$
Let us make the change of variable $(xi, tau) = (x-at,t)$, so that $partial_t = partial_tau - apartial_xi$ and $partial_x = partial_xi$. Thus, using Fubini's theorem and integration by parts,
begin{aligned}
iint_{Bbb RtimesBbb R_+} u, (phi_t + a phi_x), text d x,text d t
&= iint_{Bbb RtimesBbb R_+} u phi_tau, text d xi,text d tau \
&= iint_{Bbb R_+timesBbb R} u phi_tau, text d tau,text d xi \
&= int_{Bbb R}left[uphiright]_{tauinBbb R_+}text dxi - iint_{Bbb R_+timesBbb R} underbrace{u_tau}_{=0} phi, text d tau,text d xi \
&= -int_{Bbb R}left.(uphi)right|_{t = 0}text dx , .
end{aligned}
We have shown that the definition holds for all smooth $phi$ with compact support. Hence, $u(x,t) = g(x-at)$ is a weak solution to the Cauchy problem of the advection equation. Note that there may be a sign mistake.
$endgroup$
add a comment |
$begingroup$
Let us make the change of variable $(xi, tau) = (x-at,t)$, so that $partial_t = partial_tau - apartial_xi$ and $partial_x = partial_xi$. Thus, using Fubini's theorem and integration by parts,
begin{aligned}
iint_{Bbb RtimesBbb R_+} u, (phi_t + a phi_x), text d x,text d t
&= iint_{Bbb RtimesBbb R_+} u phi_tau, text d xi,text d tau \
&= iint_{Bbb R_+timesBbb R} u phi_tau, text d tau,text d xi \
&= int_{Bbb R}left[uphiright]_{tauinBbb R_+}text dxi - iint_{Bbb R_+timesBbb R} underbrace{u_tau}_{=0} phi, text d tau,text d xi \
&= -int_{Bbb R}left.(uphi)right|_{t = 0}text dx , .
end{aligned}
We have shown that the definition holds for all smooth $phi$ with compact support. Hence, $u(x,t) = g(x-at)$ is a weak solution to the Cauchy problem of the advection equation. Note that there may be a sign mistake.
$endgroup$
add a comment |
$begingroup$
Let us make the change of variable $(xi, tau) = (x-at,t)$, so that $partial_t = partial_tau - apartial_xi$ and $partial_x = partial_xi$. Thus, using Fubini's theorem and integration by parts,
begin{aligned}
iint_{Bbb RtimesBbb R_+} u, (phi_t + a phi_x), text d x,text d t
&= iint_{Bbb RtimesBbb R_+} u phi_tau, text d xi,text d tau \
&= iint_{Bbb R_+timesBbb R} u phi_tau, text d tau,text d xi \
&= int_{Bbb R}left[uphiright]_{tauinBbb R_+}text dxi - iint_{Bbb R_+timesBbb R} underbrace{u_tau}_{=0} phi, text d tau,text d xi \
&= -int_{Bbb R}left.(uphi)right|_{t = 0}text dx , .
end{aligned}
We have shown that the definition holds for all smooth $phi$ with compact support. Hence, $u(x,t) = g(x-at)$ is a weak solution to the Cauchy problem of the advection equation. Note that there may be a sign mistake.
$endgroup$
Let us make the change of variable $(xi, tau) = (x-at,t)$, so that $partial_t = partial_tau - apartial_xi$ and $partial_x = partial_xi$. Thus, using Fubini's theorem and integration by parts,
begin{aligned}
iint_{Bbb RtimesBbb R_+} u, (phi_t + a phi_x), text d x,text d t
&= iint_{Bbb RtimesBbb R_+} u phi_tau, text d xi,text d tau \
&= iint_{Bbb R_+timesBbb R} u phi_tau, text d tau,text d xi \
&= int_{Bbb R}left[uphiright]_{tauinBbb R_+}text dxi - iint_{Bbb R_+timesBbb R} underbrace{u_tau}_{=0} phi, text d tau,text d xi \
&= -int_{Bbb R}left.(uphi)right|_{t = 0}text dx , .
end{aligned}
We have shown that the definition holds for all smooth $phi$ with compact support. Hence, $u(x,t) = g(x-at)$ is a weak solution to the Cauchy problem of the advection equation. Note that there may be a sign mistake.
answered Aug 8 '18 at 9:58
Harry49Harry49
6,21331132
6,21331132
add a comment |
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$begingroup$
You simply need to show that $u(x,t) = g(x-at)$ satisfies the integral equation for all $phiin C_c^1(mathbb{R}times [0,infty))$. Divergence theorem and integration by parts would be useful for you.
$endgroup$
– Chee Han
Jul 27 '18 at 22:54
$begingroup$
Can we apply integration by parts and divergence theorem as g is only $L^{infty}$? Could u please give the complete proof.. I am unable to follow
$endgroup$
– Rosy
Aug 3 '18 at 8:23