Initial Value Problem and Inhomogeneous Problem Solutions for the Transport Equation
📂Partial Differential EquationsInitial Value Problem and Inhomogeneous Problem Solutions for the Transport Equation
Equation
Below partial differential equation is known as the transport equation.
ut+b⋅Du=0in Rn×(0, ∞)
Solution
Initial Value Problem
Let’s suppose the initial value problem of the transport equation is given as follows.
{ut+b⋅Duu=0=gin Rn×[0, ∞)on Rn×{t=0}
b∈Rn is a constant given in the transport equation, and g:Rn→R is given as the initial value. The problem is to obtain u. Let’s define z as follows.
z(s):=u(x+sb, t+s)(s∈R)
Then, we obtain the following.
z(−t)=u(x−tb, 0)=g(x−tb)
Also, since the value of z(s) is independent of s, the following holds.
z(−t)=z(0)=u(x, t)
Therefore, the solution is as follows.
u(x, t)=g(x−tb) (x∈Rn, t≥0)
Conversely, if there is g∈C1(Rn) satisfying u(x, t)=g(x−tb), then u∈C1 becomes a solution of (1).
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Nonhomogeneous Problem
It is the case where the term on the right-hand side is not 0 in the initial value problem.
{ut+b⋅Duu=f=gin Rn×[0, ∞)onRn×{t=0}
Regarding z defined above, if we find z˙, it is as follows.
z˙(s)=dsdz=∂x∂udsdx+∂t∂udsdt=Du(x+sb, t+s)⋅b+ut(x+sb, t+s)=f(x+sb, t+s)
Therefore, the following holds.
u(x, t)−g(x−tb)=z(0)−z(−t)=∫−t0z˙(s)ds=∫−t0f(x+sb, t+s)ds=∫0tf(x+(s−t)b, s)ds
The fourth equality holds by substituting s≡s′+t. Then, the solution of (2) is as follows.
u(x, t)=g(x−tb)+∫0tf(x+(s−t)b, s)ds(x∈Rn, t≥0)
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