Problem 4 The heated rod from Problem 3 is subject to a volumetric heating h(x) = ho in units of [Wm³], as shown in the figure below. Under the heat supply the temperature of the rod changes along x with the temperature function T(x). The temperature T(x) is governed by the following equations: d dx (g(x)) + h(x) = 0 PDE q(x) = −kdx -кат (4) Fourier's law of heat conduction where q(x) is the heat flux through the rod and k is the (constant) thermal conductivity. Both ends of the bar are in contact with a heat reservoir at zero temperature. T(x) h(x) L 8 00

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
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The heated rod from Problem 3 is subject to a volumetric heating

h(x) = h0

x

L in units of [Wm−3], as shown in the figure below. Under the

heat supply the temperature of the rod changes along x with the

temperature function T (x). The temperature T (x) is governed by the

d

following equations:

dx (q(x)) + h(x) = 0 PDE

q(x) =−k dT

dx Fourier’s law of heat conduction (4)

where q(x) is the heat flux through the rod and k is the (constant)

thermal conductivity. Both ends of the bar are in contact with a heat

reservoir at zero temperature.

Determine:

1. Appropriate BCs for this physical problem.

2. The temperature function T (x).

3. The heat flux function q(x).

Side Note: Please see that both ends of bar are in contact with a heat reservoir at zero temperature so the boundary condition at the right cannot be du/dx=0 because its not thermally insulated. Thank you 

 

Problem 4
The heated rod from Problem 3 is subject to a volumetric heating
h(x) = ho in units of [Wm³], as shown in the figure below. Under the
heat supply the temperature of the rod changes along x with the
temperature function T(x). The temperature T(x) is governed by the
following equations:
d
dx
(g(x)) + h(x) = 0 PDE
q(x) = −kdx
-кат
(4)
Fourier's law of heat conduction
where q(x) is the heat flux through the rod and k is the (constant)
thermal conductivity. Both ends of the bar are in contact with a heat
reservoir at zero temperature.
T(x)
h(x)
L
8
00
Transcribed Image Text:Problem 4 The heated rod from Problem 3 is subject to a volumetric heating h(x) = ho in units of [Wm³], as shown in the figure below. Under the heat supply the temperature of the rod changes along x with the temperature function T(x). The temperature T(x) is governed by the following equations: d dx (g(x)) + h(x) = 0 PDE q(x) = −kdx -кат (4) Fourier's law of heat conduction where q(x) is the heat flux through the rod and k is the (constant) thermal conductivity. Both ends of the bar are in contact with a heat reservoir at zero temperature. T(x) h(x) L 8 00
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