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N UMERICAL S IMULATIONS Motolani Olarinre Ivana Seric Mandeep Singh.

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Presentation on theme: "N UMERICAL S IMULATIONS Motolani Olarinre Ivana Seric Mandeep Singh."— Presentation transcript:

1 N UMERICAL S IMULATIONS Motolani Olarinre Ivana Seric Mandeep Singh

2 I NTRODUCTION

3 M ETHOD AND BC’ S

4 N UMERICAL R ESULTS Types of wave profiles: -Traveling wave solution -Convective instability -Absolute instability Figure: Flow down the vertical plane (t=10). From top to bottom, N=16, 22, 27.

5 S TABLE TRAVELING WAVE SOLUTION

6 Flow down the vertical plane (N=16). From top to bottom, t=0, 40, 80, 120.

7 C ONVECTIVE INSTABILITY Figure: N=22, flow down the vertical. From top to bottom, t=0, 40, 80, 120.

8 C ONVECTIVE INSTABILITY

9 A BSOLUTE INSTABILITY Figure: N=27, absolute instability. From top to bottom, t=0, 40, 80, 120.

10 A BSOLUTE INSTABILITY

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12 S PEED OF THE LEFT BOUNDARY NumLSANumLSA 18.617.7925.4325.44 24.424.1330.630.46

13 NUMERICS

14 F INITE D IFFERENCE D ISCRETIZATION P ROCEDURE

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16 O UR S IMULATIONS We ran simulations in FORTRAN using the following parameters: C = 1, B = 0, N = 10, U = 1, b = 0.1, beta = 1. These parameters indicate a liquid crystal flowing down a vertical surface (90 degree angle) The output from our simulations were plotted and analyzed using MATLAB

17 We ran simulations for two distinct cases: – Constant Flux: Uses a semi-infinite hyperbolic tangent profile for its initial condition. Simulates a case where an infinite volume of liquid is flowing. – Constant Volume: Uses a square hyperbolic tangent profile for its initial condition. Simulates a case where a drop is flowing. O UR S IMULATIONS

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19 G ROWTH R ATE A NALYSIS

20

21

22 80.7854 100.6283 120.5236 140.4488 160.3927 180.3491 200.3142

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25 G ROWTH R ATE A NALYSIS


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