2. Solve the one-dimensional heat equation problem for a unit length bar with insulated ends with...
* Exercise 4: Let k,l 〉 0. The temperature of a rod insulated at the ends with an expo- nentially decreasing heat source in it satisfies the following problem: ux (0, t) u(z,0) 0 = ux (1, t), φ(z) Find the solution to this problem by writing u as a cosine series: Ao(t) u(x, t) An(t) cos and determine limt-Hou(z, t
(a) Consider the one-dimensional heat equation for the temperature u(x, t), Ou,02u where c is the diffusivity (i) Show that a solution of the form u(x,t)-F )G(t) satisfies the heat equation, provided that 护F and where p is a real constant (ii) Show that u(x,t) has a solution of the form (,t)A cos(pr)+ Bsin(p)le -P2e2 where A and B are constants (b) Consider heat flow in a metal rod of length L = π. The ends of the rod, at...
(a) The heat flux through the faces at the ends of bar is found to be proportional to un au/an at the ends. If the bar is perfectly insulated, also at the ends x 0 and x L are adiabatic conditions, Q1 ux(0, t) = 0 0 (2'7)*n prove that the solution of the heat transfer problem above (adiabatic conditions at both ends) gives as, 2 an: nnx u(x, t) Ao t An cos n-1 where Ao and An are...
Problem 3 Using Fourier series expansion, solve the heat conduction equation in one dimension a?т ат ax2 де with the Dirichlet boundary conditions: T T, if x 0, and T temperature distribution is given by: T(x, 0) -f(x) T, if x L. The initial 0 = *First find the steady state temperature distribution under the given boundary conditions. The steady form solution has the form (x)-C+C2x *Then write for the full solution T(x,t)=To(x)+u(x,t) with u(x,t) obeying the boundary contions U(0,t)...
Solve the heat equation ut = 10uct for a rod of length 1 with both ends insulated for all time (zero Neumann boundary conditions), if the initial temperature is given by (2) = x+sin ax. First, formulate the mathematical problem and complete the three steps as described. Mathematical Formulation Step 1: Derive an expression for all nontrivial product (separated) solutions including an eigenvalue problem satisfying the boundary conditions Step 2: Solve the eigenvalue problem Step 3: Use the superposition principle...
PDE. Please show all steps in detail. 2. Consider the 1D heat equation in a rod of length with diffusion constant Suppose the left endpoint is convecting (in obedience to Newton's Law of Cooling with proportionality constant K-1) with an outside medium which is 5000. while the right endpoint is insulated. The initial temperature distribution in the rod is given by f(a)- 2000 -0.65 300, 0<
This is a question about Partial differential equation - Heat equation. Please help solving part (a) and show clear explanations. Thanks! =K х 7. The temperature T(2,t) in an insulated rod of length L and diffusivity k is given by the heat equation ОТ 22T 0 < x < L. at Əx2' Initially this rod is at constant temperature To, and immediately after t=0 the temperature at x = L is suddenly increased to T1. The temperature at x =...
please, please, explain the process and step by step how to solve this problem, I want to get the logic and process: >> Do not simplify the answer. I already saw other answers and still do not get the process how to solve it<< 1. In class we found that the Fourier series of a unit amplitude square wave of period 2 seconds was given by x(t) = Σ 그etjnitt HTT odd (a) Show that this series can be rewritten...
2. Consider the heat equation on a bounded domain with a zero heat-flux condition, 0<a <1 t > 0, u(z,0) = 2(1-2), (0, t) = 0, 14(1, t) = 0, t >0, t > 0, where σ > 0 is a constant. Such an equation is a model for the distribution of head throughout a rod which is thermally insulated on both ends. (a) Find the solution of the above PDE using separation of variables. You may use anything we...
Problem 2 Consider the one dimensional version of the heat PDE in Problem1 2 0x2 a(0, z) = uo(z) = e-r2. (a) Write down the Fourier transformed version of (2). Then, find the solution of this transformed version u(t,)-((,) (b) Invert the solution in part (a) to get the solution, u(t, x)-F-(u)(t, x), to (2) Problem 2 Consider the one dimensional version of the heat PDE in Problem1 2 0x2 a(0, z) = uo(z) = e-r2. (a) Write down the...