For 0 x π , 0S9, π , and 120 , solve the 2-D wave equation subject to the following conditions. u(0,y,t)-0, u(T.yt):0, u(x,0,) u(x,π, t) 0, 0 Boundary condition: C11 1 u(x),0)-sin(x)sin(2y) + sin(2x)sin(4y), 0 at It=0 Initial condition:
For 0 x π , 0S9, π , and 120 , solve the 2-D wave equation subject to the following conditions. u(0,y,t)-0, u(T.yt):0, u(x,0,) u(x,π, t) 0, 0 Boundary condition: C11 1 u(x),0)-sin(x)sin(2y) + sin(2x)sin(4y), 0 at It=0 Initial condition:
ou(x.y)@uxy)o for the temperature 2. Solve Laplace's equation distribution in a rectangular plate 0sx s1, 0sysl subject to the following conditions. (a) u(0,y)-0, uy)-0, u(x,0)-fx), u(x,I)-0 au (x,y) x, y y- o
ou(x.y)@uxy)o for the temperature 2. Solve Laplace's equation distribution in a rectangular plate 0sx s1, 0sysl subject to the following conditions. (a) u(0,y)-0, uy)-0, u(x,0)-fx), u(x,I)-0 au (x,y) x, y y- o
A sheet of metal coincides with the square in the xy-plane whose vertices (0, O), (1 0), (1, 1) and (0, 1). The two faces of the sheet are insulated, and the sheet is so thin that heat flow in it can be regarded as two-dimensional. The edges parallel to the x- axis are insulated, and the left-hand edge is maintained at the constant temperature O. If the temperature distribution u(1, y) f(y) is maintained along the right-hand edge, Set...
Solve Laplace's equation, \(\frac{\partial^{2} u}{\partial x^{2}}+\frac{\partial^{2} u}{\partial y^{2}}=0,0<x<a, 0<y<b\), (see (1) in Section 12.5) for a rectangular plate subject to the given boundary conditions.$$ \begin{gathered} \left.\frac{\partial u}{\partial x}\right|_{x=0}=u(0, y), \quad u(\pi, y)=1 \\ u(x, 0)=0, \quad u(x, \pi)=0 \\ u(x, y)=\square+\sum_{n=1}^{\infty}(\square \end{gathered} $$
Consider the steady temperature T (2,y) in a rectangular plate that occupies 0 <<< 9 and 0 <y<5, which is heated at constant temperature 150 at 9 and 0 along its other three sides. (a) For separation solutions T(1,y) = F(x)G(y), you are given that admissible F(1) are the eigenfunctions Fn (1) = sinh(An I) for n=1,2,... and G(y) are the eigenfunctions Gn(y) = sin(Any) for n=1,2,... A for In = (b) The solution is the superposition T(z,y) = an...
7.4 Solve the Laplace equation Δ11-0 in the square 0 < x, y < π, subject to the bound- ary condition 11(0, y) u(T, y) = 0. 11(x, 0) = 11(x, π) = 1, = 1/(π, y) =
7.4 Solve the Laplace equation Δ11-0 in the square 0
The motion of a string with fixed ends in a viscous medium is described by: together with boundary conditions: u(0,t) 0 and u(2, t)0 and initially: u(z,0-sin(nz/2) and ut(z, 0)--sin(2πχ). (a) If u(x, t) - X(x)T(t) find the ordinary differential equations satisfied by X and T e ordinary different (c) Determine u(x, t).
The motion of a string with fixed ends in a viscous medium is described by: together with boundary conditions: u(0,t) 0 and u(2, t)0 and initially: u(z,0-sin(nz/2)...
25 points) Find the solution of the Laplace equation ur the domain 0-x-π and 0-y-T. The boundary condition at the left boundary is given by u(0, y)-sin(y/2). The boundary conditions at al other boundaries are zero. Express the solution as an infinite series = 0, over
10. [18 Marks] Using separation of variables, solve Laplace's equation for {(x,y): 0 < x < 2,0 < y < 2), subject to the boundary conditions 0 (0, y) = d(x, 2) 6 + cos(nz) = In your solution, you must consider all three cases for the separation constant λ.
10. [18 Marks] Using separation of variables, solve Laplace's equation for {(x,y): 0
2. Solve for the bounded solution of Laplace's equation v2T=0 in the UHP: [2] < 0, y > 0 with the following boundary conditions given on y = 0: T(x,0) = {A on x < l1, B on li < x < l2,C on x > la} A, B, C are real constants.