Pde Rectangular 4B56D5
1. **Problem Statement:**
Solve the PDE $$\frac{\partial u}{\partial t} = \frac{\partial u}{\partial x} + \frac{\partial u}{\partial y} + \sin t \cos x \cos y$$
with boundary conditions:
$$u_x(0,y,t) = A, \quad u_x(\pi,y,t) = 0, \quad u(x,\infty,t) = u(x,\pi,t) = 0$$
and initial conditions:
$$u(x,y,0) = \alpha(x,y), \quad u_t(x,y,0) = \beta(x,y)$$
2. **Formula and Important Rules:**
This is a first-order PDE with mixed spatial derivatives and a source term depending on $t$, $x$, and $y$.
We use the method of characteristics or separation of variables combined with Duhamel's principle for the nonhomogeneous term.
3. **Step-by-step Solution Approach:**
- Rewrite PDE as:
$$\frac{\partial u}{\partial t} - \frac{\partial u}{\partial x} - \frac{\partial u}{\partial y} = \sin t \cos x \cos y$$
- Homogeneous part:
$$\frac{\partial u}{\partial t} - \frac{\partial u}{\partial x} - \frac{\partial u}{\partial y} = 0$$
- Characteristic equations:
$$\frac{dt}{1} = \frac{dx}{-1} = \frac{dy}{-1}$$
which imply along characteristics:
$$x + t = \text{const}, \quad y + t = \text{const}$$
- General solution to homogeneous PDE is a function of $x+t$ and $y+t$:
$$u_h = F(x+t,y+t)$$
- For the nonhomogeneous term, use variation of parameters or Duhamel's principle:
4. **Particular solution guess:**
Try a solution of form:
$$u_p = g(t) \cos x \cos y$$
Substitute into PDE:
$$g'(t) \cos x \cos y - 0 - 0 = \sin t \cos x \cos y$$
which simplifies to:
$$g'(t) = \sin t$$
Integrate:
$$g(t) = -\cos t + C$$
5. **Complete solution:**
$$u = F(x+t,y+t) - \cos t \cos x \cos y + C \cos x \cos y$$
6. **Apply boundary conditions:**
- At $x=0$:
$$u_x(0,y,t) = A$$
Calculate derivative:
$$u_x = F_x(x+t,y+t) - \cos t (-\sin x) \cos y + C (-\sin x) \cos y$$
At $x=0$, $\sin 0=0$, so:
$$u_x(0,y,t) = F_x(t,y+t) = A$$
- At $x=\pi$:
$$u_x(\pi,y,t) = F_x(\pi+t,y+t) = 0$$
- At $y=\pi$ and $y=\infty$:
$$u(x,\pi,t) = F(x+t,\pi+t) - \cos t \cos x \cos \pi + C \cos x \cos \pi = 0$$
Since $\cos \pi = -1$,
$$F(x+t,\pi+t) + \cos t \cos x - C \cos x = 0$$
7. **Initial conditions:**
At $t=0$:
$$u(x,y,0) = F(x,y) - \cos 0 \cos x \cos y + C \cos x \cos y = \alpha(x,y)$$
$$u_t(x,y,0) = F_t(x,y) + \sin 0 \cos x \cos y = \beta(x,y)$$
Since $\sin 0=0$,
$$u_t(x,y,0) = F_t(x,y) = \beta(x,y)$$
8. **Summary:**
- $F$ and $C$ are determined by boundary and initial conditions.
- The solution combines a traveling wave $F(x+t,y+t)$ and a particular solution involving $\cos t \cos x \cos y$.
This approach outlines the method to solve the PDE with given BC and IC.
**Final answer:**
$$u(x,y,t) = F(x+t,y+t) - \cos t \cos x \cos y + C \cos x \cos y$$
where $F$ and $C$ satisfy the boundary and initial conditions.