Computational Fluid Dynamics Questions and Answers – Approaches for Non-uniform Time Steps

This set of Computational Fluid Dynamics Problems focuses on “Approaches for Non-uniform Time Steps”.

1. Discretization of the transient term is not affected by uniform or non-uniform grids when _________
a) the scheme is downwind
b) the scheme is upwind
c) the scheme is first-order
d) the scheme is second-order
View Answer

Answer: c
Explanation: Since the second-order schemes use a stencil with two time-steps in the same direction, only the second-order schemes are affected by the non-uniformity of the grids. The first-order schemes are not affected.

2. For which of these schemes is the interpolation profile need not be modified for the non-uniform transient grid?
a) Downwind scheme
b) Upwind scheme
c) Crank-Nicolson scheme
d) second-order schemes
View Answer

Answer: c
Explanation: For all the second-order schemes, the interpolation profile has to be modified when the transient grid is non-uniform. But this is not the case when the Crank-Nicolson scheme is used. There is no change in the interpolation profile needed here.

3. Which of these characteristics of the Crank-Nicolson scheme is affected by the non-uniform transient grids?
a) Consistency
b) Convergence
c) Stability
d) Accuracy
View Answer

Answer: d
Explanation: When the Crank-Nicolson scheme is used on the non-uniform transient grids, for each of the two steps, a different time-step is used. So, the spatial derivative is not at the centre of the temporal elements. Therefore, the accuracy is affected.
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4. Which of these statements is correct about the variable time-steps?
a) The finite volume and finite difference schemes do not yield equivalent algebraic equations
b) The finite volume scheme yields equivalent algebraic equations irrespective of the non-uniformity
c) The finite difference scheme yields equivalent algebraic equations irrespective of the non-uniformity
d) All the second-order schemes result in the same algebraic equation when the grid is non-uniform
View Answer

Answer: a
Explanation: The finite volume and finite difference schemes yield equivalent algebraic equations when the transient grid is uniform. If the grid is non-uniform, the algebraic equations are not the same.

5. If the Crank-Nicolson scheme is used with the finite difference approach to get the discretized equation of the transient term with the non-uniform grid, what is the central coefficient of the previous time-step?
(Note: ρ is the density and V the volume).
a) \(\frac{\Delta t-\Delta t^o}{\Delta t+\Delta t^o}\rho_C V_C\)
b) \(\frac{\Delta t-\Delta t^o}{\Delta t+\Delta t^o}\rho_C^o V_C\)
c) \(\frac{\Delta t-\Delta t^o}{\Delta t+\Delta t^o}\rho_C^o\)
d) \(\frac{\Delta t+\Delta t^o}{\Delta t-\Delta t^o}\rho_C^o V_C\)
View Answer

Answer: b
Explanation: When the transient grid system is not uniform,
Δt≠Δ t°
Therefore, when the Crank-Nicolson scheme is used, density varies but the volume does not vary.
\(a_C^o=\frac{\Delta t-\Delta t^o}{\Delta t+\Delta t^o}\rho_C^o V_C\) This becomes zero when a uniform transient grid is used.

6. If the Crank-Nicolson scheme is used with the finite difference approach to get the discretized equation of the transient term with the non-uniform grid, what is the central coefficient of the second previous time-step?
(Note: ρ is the density and V the volume).
a) \(\frac{\Delta t^o}{\Delta t(\Delta t+\Delta t^o)}\rho_C^{oo}V_C\)
b) \(\frac{\Delta t(\Delta t+\Delta t^o)}{\Delta t×\Delta t^o}\rho_C^{oo}V_C\)
c) \(\frac{\Delta t+2\Delta t^o}{(\Delta t+\Delta t^o)}\rho_C^{oo}V_C\)
d) \(\frac{\Delta t}{\Delta t^o(\Delta t+\Delta t^o)}\rho_C^{oo}V_C\)
View Answer

Answer: d
Explanation: While using the Crank-Nicolson scheme, the previous and the next time steps are t+Δt and t-Δ t°. Using these in the semi-discretized equation, the coefficient of the second previous time-step is
\(a_C^{oo}=\frac{\Delta t}{\Delta t^o(\Delta t+\Delta t^o)}\rho_C^{oo}V_C\).

7. If the Adams-Moulton scheme is used with the finite difference approach to get the discretized equation of the transient term with the non-uniform grid, what is the central coefficient of the current time-step?
(Note: ρ is the density and V the volume).
a) \((\frac{1}{\Delta t^o}+\frac{1}{\Delta t+\Delta t^o}) \rho_C V_C\)
b) \((\frac{1}{\Delta t}+\frac{1}{\Delta t^{oo}+\Delta t^o}) \rho_C V_C\)
c) \((\frac{1}{\Delta t}+\frac{1}{\Delta t+\Delta t^{oo}})\rho_C V_C\)
d) \((\frac{1}{\Delta t}+\frac{1}{\Delta t+\Delta t^o})\rho_C V_C\)
View Answer

Answer: d
Explanation: The Adams-Moulton scheme uses the time-steps Δt-Δt° and Δt-Δt°. Applying these time-steps, the central coefficient of the current time-step is given by
\((\frac{1}{\Delta t}+\frac{1}{\Delta t+\Delta t^o})\rho_C V_C\).
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8. Which of these is correct for the non-uniform time-steps?
(Note: δt is the distance between the centroids of two temporal elements. Δt is the size of a temporal element. The superscript o indicates the older time step).
a) \(\delta t=\frac{(\Delta t-\Delta t^o)}{2}\)
b) \(\delta t=\frac{(\Delta t+\Delta t^o)}{2}\)
c) δt=Δt
d) δt=Δt°
View Answer

Answer: b
Explanation: For the variable time-steps, \(\delta t=\frac{(\Delta t+\Delta t^o)}{2}\) as the size of the temporal element is not the same. For the uniform transient grids, this reduces to δt=Δt as Δ t=Δt°.

9. The general discretised form of the transient term using the finite volume approach is
FluxT=FluxC ΦC+FluxC°ΦC°+FluxV.
The superscript o indicates the older time step. If the Crank-Nicolson method is used with non-uniform grids, what is FluxV?
a) \(-\frac{\Delta t^{oo}}{\Delta t^o}\frac{\rho_c^{oo} V_C\phi_c^{oo}}{\Delta t}\)
b) \(\frac{\Delta t^{oo}}{\Delta t^o+\Delta t^{oo}}\frac{\rho_c^{oo} V_C \phi_c^{oo}}{\Delta t}\)
c) \(-\frac{\Delta t^{oo}}{\Delta t^o+\Delta t^{oo}}\frac{\rho_c^{oo} V_C \phi_c^{oo}}{\Delta t}\)
d) \(\frac{\Delta t^{oo}}{\Delta t^o}\frac{\rho_c^{oo} V_C \phi_c^{oo}}{\Delta t}\)
View Answer

Answer: c
Explanation: The Crank-Nicolson scheme uses the average of the two central values to get the values at the interface. Using this with the non-uniform time-steps,
FluxV=-\(-\frac{\Delta t^{oo}}{\Delta t^o+\Delta t^{oo}}\frac{\rho_c^{oo} V_C \phi_c^{oo}}{\Delta t}\).
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10. Which of these statements is correct regarding the Adams-Moulton scheme used on the non-uniform grids?
a) The current central coefficient for the finite difference and the finite volume schemes are the same
b) The current central coefficient for the uniform and the non-uniform grid is the same
c) The variation in time-steps does not result in any change
d) There is no variation in the values when the grid is uniform
View Answer

Answer: a
Explanation: For the finite difference approach,
\(a_c=(\frac{1}{\Delta t}+\frac{1}{\Delta t+\Delta t^o})\rho_C V_C\)
For the finite volume approach, the central coefficient is
FluxC=\((\frac{1}{\Delta t}+\frac{1}{\Delta t+\Delta t^o})\rho_C V_C\)
These two are the same irrespective of the approach.

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Manish Bhojasia, a technology veteran with 20+ years @ Cisco & Wipro, is Founder and CTO at Sanfoundry. He lives in Bangalore, and focuses on development of Linux Kernel, SAN Technologies, Advanced C, Data Structures & Alogrithms. Stay connected with him at LinkedIn.

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