Elements Of Electromagnetics
Elements Of Electromagnetics
7th Edition
ISBN: 9780190698614
Author: Sadiku, Matthew N. O.
Publisher: Oxford University Press
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Derive from the 4.93 equation to the 4.94 equation

A simple implicit scheme for the heat equation was proposed by Laasonen (1949). The
algorithm for this scheme is
u+¹-u
At
Ut αuxx =
u+1-2u+¹+₁+1
= α-
If we make use of the central-difference operator
-
we can rewrite Equation 4.92 in the simpler form:
u₁¹uj
At
8u =u+1-2u+u₁_₁
(Ax)²
a(Ax)²
12
= α
8u+1
(4x)²
This scheme has first-order accuracy with a T.E. of O[(At)², (Ax)² ] and is unconditionally
stable. Upon examining Equation 4.93, it is apparent that a tridiagonal system of linear
algebraic equations must be solved at each time level n +1.
The modified equation for this scheme is
Uxxxx
+ [ { α² (At)² + 1 2 α²³At(^x)² -
+
12
___a (4x) *] ¹.*
360
(4.92)
+..
(4.93)
(4.94)
expand button
Transcribed Image Text:A simple implicit scheme for the heat equation was proposed by Laasonen (1949). The algorithm for this scheme is u+¹-u At Ut αuxx = u+1-2u+¹+₁+1 = α- If we make use of the central-difference operator - we can rewrite Equation 4.92 in the simpler form: u₁¹uj At 8u =u+1-2u+u₁_₁ (Ax)² a(Ax)² 12 = α 8u+1 (4x)² This scheme has first-order accuracy with a T.E. of O[(At)², (Ax)² ] and is unconditionally stable. Upon examining Equation 4.93, it is apparent that a tridiagonal system of linear algebraic equations must be solved at each time level n +1. The modified equation for this scheme is Uxxxx + [ { α² (At)² + 1 2 α²³At(^x)² - + 12 ___a (4x) *] ¹.* 360 (4.92) +.. (4.93) (4.94)
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