(e) Show that v(x, t) = u(x, t) — uĘ(x, t) is solution of a homogeneous problem (with a different initial condition) and solve it using the method of separation of variables and the superposition principle. The solution has the form 00 v(x,t) = Go(t) + Σ Gn(t) cos(nлx) n=1 Enter the functions Go (t) and Gn(t) (in that order) into the answer box below, separated with a comma. (f) The solution u(x, t) of the original problem, written as a cosine Fourier series with coefficients that are functions of t, has the form 80 u(x,t) = H₁(t) + Σ H₂(t) cos(nлx) n=1 Enter the functions Ho(t) and Hn(t) (in that order) into the answer box below, separated with a comma. : Consider the following heat equation on a rod (which includes heat loss through the lateral side and fixed heat flow on the boundary): ди at 22 и = 2х2 - 9u, 0 < x < 1, t > 0, subject to the boundary conditions ux(0,t) = 3, ux(1,t) = 18, t > 0, and the initial condition u(x, 0) = 0, 0 < x < 1. (a) Find the equilibrium solution uĘ(x) for this problem by solving a certain boundary value problem on (0, 1). (b) Use integration by parts and the given boundary conditions that uĘ(x) satisfies to compute A₁ = √√√u (x ) d x Ao Enter Ao. (Do not use the explicit formula for uĚ (x) obtained in part (a).) (c) Use integration by parts and the given boundary conditions that uĘ (x) satisfies to show that Lug (x) cos(nлx) dx ) cos(nлx) dx = A + Bn² uд(x) cos(nлx) dx, n ≥ 1, (1) for some constants B and An. (Do not use the explicit formula for uE (x) obtained in part (a).) Enter the values of B and An (in that order) into the answer box below, separated with a comma. (d) Use the differential equation that uд(x) satisfies together with the results obtained in (b) and (c) to deduce the Fourier cosine series representation for uд(x) on (0, 1) which is of the form 2 + 80 Σan cos(ηπx). n =1 Enter the values of ao and an (in that order) into the answer box below, separated with a comma. - (e) Show that v(x,t) = u(x,t) – u£ (x, t) is solution of a homogeneous problem (with a different initial condition) and solve it using the method of separation of variables and the superposition principle. The solution has the form

Calculus: Early Transcendentals
8th Edition
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Author:James Stewart
Publisher:James Stewart
Chapter1: Functions And Models
Section: Chapter Questions
Problem 1RCC: (a) What is a function? What are its domain and range? (b) What is the graph of a function? (c) How...
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Please utilizing the solutions to the previous sub questions, solve and write out explicitly the values of the solutions to E and F i.e. Go(t), Gn(t), Ho(t), Hn(t)

(e) Show that v(x, t) = u(x, t) — uĘ(x, t) is solution of a homogeneous problem (with a different initial condition)
and solve it using the method of separation of variables and the superposition principle. The solution has the
form
00
v(x,t) = Go(t) + Σ Gn(t) cos(nлx)
n=1
Enter the functions Go (t) and Gn(t) (in that order) into the answer box below, separated with a comma.
(f) The solution u(x, t) of the original problem, written as a cosine Fourier series with coefficients that are
functions of t, has the form
80
u(x,t) = H₁(t) + Σ H₂(t) cos(nлx)
n=1
Enter the functions Ho(t) and Hn(t) (in that order) into the answer box below, separated with a comma.
Transcribed Image Text:(e) Show that v(x, t) = u(x, t) — uĘ(x, t) is solution of a homogeneous problem (with a different initial condition) and solve it using the method of separation of variables and the superposition principle. The solution has the form 00 v(x,t) = Go(t) + Σ Gn(t) cos(nлx) n=1 Enter the functions Go (t) and Gn(t) (in that order) into the answer box below, separated with a comma. (f) The solution u(x, t) of the original problem, written as a cosine Fourier series with coefficients that are functions of t, has the form 80 u(x,t) = H₁(t) + Σ H₂(t) cos(nлx) n=1 Enter the functions Ho(t) and Hn(t) (in that order) into the answer box below, separated with a comma.
: Consider the following heat equation on a rod (which includes heat loss through the lateral side and fixed heat
flow on the boundary):
ди
at
22 и
=
2х2
- 9u, 0 < x < 1, t > 0,
subject to the boundary conditions
ux(0,t)
=
3, ux(1,t) = 18, t > 0,
and the initial condition
u(x, 0) = 0, 0 < x < 1.
(a) Find the equilibrium solution uĘ(x) for this problem by solving a certain boundary value problem on (0, 1).
(b) Use integration by parts and the given boundary conditions that uĘ(x) satisfies to compute
A₁ = √√√u (x ) d x
Ao
Enter Ao. (Do not use the explicit formula for uĚ (x) obtained in part (a).)
(c) Use integration by parts and the given boundary conditions that uĘ (x) satisfies to show that
Lug (x) cos(nлx) dx
) cos(nлx) dx = A + Bn²
uд(x) cos(nлx) dx, n ≥ 1, (1)
for some constants B and An. (Do not use the explicit formula for uE (x) obtained in part (a).) Enter the values
of B and An (in that order) into the answer box below, separated with a comma.
(d) Use the differential equation that uд(x) satisfies together with the results obtained in (b) and (c) to deduce the
Fourier cosine series representation for uд(x) on (0, 1) which is of the form
2
+
80
Σan cos(ηπx).
n =1
Enter the values of ao and an (in that order) into the answer box below, separated with a comma.
-
(e) Show that v(x,t) = u(x,t) – u£ (x, t) is solution of a homogeneous problem (with a different initial condition)
and solve it using the method of separation of variables and the superposition principle. The solution has the
form
Transcribed Image Text:: Consider the following heat equation on a rod (which includes heat loss through the lateral side and fixed heat flow on the boundary): ди at 22 и = 2х2 - 9u, 0 < x < 1, t > 0, subject to the boundary conditions ux(0,t) = 3, ux(1,t) = 18, t > 0, and the initial condition u(x, 0) = 0, 0 < x < 1. (a) Find the equilibrium solution uĘ(x) for this problem by solving a certain boundary value problem on (0, 1). (b) Use integration by parts and the given boundary conditions that uĘ(x) satisfies to compute A₁ = √√√u (x ) d x Ao Enter Ao. (Do not use the explicit formula for uĚ (x) obtained in part (a).) (c) Use integration by parts and the given boundary conditions that uĘ (x) satisfies to show that Lug (x) cos(nлx) dx ) cos(nлx) dx = A + Bn² uд(x) cos(nлx) dx, n ≥ 1, (1) for some constants B and An. (Do not use the explicit formula for uE (x) obtained in part (a).) Enter the values of B and An (in that order) into the answer box below, separated with a comma. (d) Use the differential equation that uд(x) satisfies together with the results obtained in (b) and (c) to deduce the Fourier cosine series representation for uд(x) on (0, 1) which is of the form 2 + 80 Σan cos(ηπx). n =1 Enter the values of ao and an (in that order) into the answer box below, separated with a comma. - (e) Show that v(x,t) = u(x,t) – u£ (x, t) is solution of a homogeneous problem (with a different initial condition) and solve it using the method of separation of variables and the superposition principle. The solution has the form
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