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use an explicit scheme to solve the equation (using concentration C(x,t)). the flow velocity is constant, namely U = 0.5 m/s; channel length 1000 m. Use Δx = 100 m; Δt = 100 seconds. at t=0, the channel's extended concentration is zero (C(x,0) = 0). The boundary conditions at all times at the upstream and downstream ends of the channel are 2 and 0 respectively. The count is carried out until time 5

use an explicit scheme to solve the equation (using concentration C(x,t)). the flow velocity is constant, namely U = 0.5 m/s; channel length 1000 m. Use Δx = 100 m; Δt = 100 seconds. at t=0, the channel's extended concentration is zero (C(x,0) = 0). The boundary conditions at all times at the upstream and downstream ends of the channel are 2 and 0 respectively. The count is carried out until time 5

Elements Of Electromagnetics
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
Problem 1.1MA
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use an explicit scheme to solve the equation (using concentration C(x,t)). the flow velocity is constant, namely U = 0.5 m/s; channel length 1000 m. Use Δx = 100 m; Δt = 100 seconds. at t=0, the channel's extended concentration is zero (C(x,0) = 0). The boundary conditions at all times at the upstream and downstream ends of the channel are 2 and 0 respectively. The count is carried out until time 5.
C at Cunak. DC at +U ac 2x + U dr² untuk koefisien difusi K=0, persamaan di atas menjadi: persamaan yang diselesaikan = ac dx K a²c 2 = 0
Transcribed Image Text:C at Cunak. DC at +U ac 2x + U dr² untuk koefisien difusi K=0, persamaan di atas menjadi: persamaan yang diselesaikan = ac dx K a²c 2 = 0
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