The general form of the element stiffness matrix system, with nodes indexed by i and j, is given as, AE 4² [1₁ 7] {u} = {√2, N. (a)l(a)x) L to form (2) where F0 and f(1) denote boundary forces at positions x = 0 and x = 1, respectively. Form the two basis functions for element 2, and evaluate the right hand side vector of the matrix system 2 to form the local system of equations for element 2. Then use the local system for element 1 given by (3) + = N₁(x)l(x)dx] {N;(1)ƒ(1) – N₂(0)F0}' AE FO £2500 [11] {2}-{25 L -1 2500 le the global "
The general form of the element stiffness matrix system, with nodes indexed by i and j, is given as, AE 4² [1₁ 7] {u} = {√2, N. (a)l(a)x) L to form (2) where F0 and f(1) denote boundary forces at positions x = 0 and x = 1, respectively. Form the two basis functions for element 2, and evaluate the right hand side vector of the matrix system 2 to form the local system of equations for element 2. Then use the local system for element 1 given by (3) + = N₁(x)l(x)dx] {N;(1)ƒ(1) – N₂(0)F0}' AE FO £2500 [11] {2}-{25 L -1 2500 le the global "
Principles of Heat Transfer (Activate Learning with these NEW titles from Engineering!)
8th Edition
ISBN:9781305387102
Author:Kreith, Frank; Manglik, Raj M.
Publisher:Kreith, Frank; Manglik, Raj M.
Chapter3: Transient Heat Conduction
Section: Chapter Questions
Problem 3.4P
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