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This section includes 10 Mcqs, each offering curated multiple-choice questions to sharpen your Computational Fluid Dynamics knowledge and support exam preparation. Choose a topic below to get started.
1. |
The numerical diffusion and numerical anti-diffusion terms are equal for the first-order Euler scheme are equal in magnitude when __________ |
A. | the courant number of diffusion is equal to one |
B. | the courant number of diffusion is equal to two |
C. | the courant number of convection is equal to one |
D. | the courant number of convection is equal to two |
Answer» D. the courant number of convection is equal to two | |
2. |
According to the first-order explicit Euler scheme, the value at time-step t- ( frac{ Delta t}{2} ) is approximated to be equal to the value at __________ |
A. | t+ ( frac{ Delta t}{2} ) |
B. | t |
C. | t- t |
D. | t+ t |
Answer» C. t- t | |
3. |
The extra term added while discretizing the transient term of a flow with density and flow variable using the first-order explicit Euler scheme is _________ |
A. | ( Delta t frac{ partial^2( rho phi)}{ partial t^2} ) |
B. | (- Delta t frac{ partial^2( rho phi)}{ partial t^2} ) |
C. | ( frac{ Delta t}{2} frac{ partial^2( rho phi)}{ partial t^2} ) |
D. | (- frac{ Delta t}{2} frac{ partial^2( rho phi)}{ partial t^2} ) |
Answer» E. | |
4. |
When the first-order implicit Euler scheme is unconditionally stable, the solution is ________ |
A. | stationary for large time-steps |
B. | oscillatory for large time-steps |
C. | stationary for small time-steps |
D. | oscillatory for small time-steps |
Answer» B. oscillatory for large time-steps | |
5. |
The first-order implicit Euler schemes to discretize the transient term creates ________ |
A. | cross-flow diffusion |
B. | cross-diffusion |
C. | numerical anti-diffusion |
D. | numerical diffusion |
Answer» E. | |
6. |
Which of these equations is the discretized form of the transient term using the first-order implicit Euler scheme? |
A. | ( frac{( rho_C phi_C)^t-( rho_C phi_C)^{t+ Delta t}}{ Delta t} V_C+L( phi_C^t) ) |
B. | ( frac{( rho_C phi_C)^t-( rho_C phi_C)^{t- Delta t}}{ Delta t} V_C+L( phi_C^t) ) |
C. | ( frac{( rho_C phi_C)^t+( rho_C phi_C)^{t+ Delta t}}{ Delta t} V_C+L( phi_C^t) ) |
D. | ( frac{( rho_C phi_C)^t+( rho_C phi_C)^{t- Delta t}}{ Delta t} V_C+L( phi_C^t) ) |
Answer» C. ( frac{( rho_C phi_C)^t+( rho_C phi_C)^{t+ Delta t}}{ Delta t} V_C+L( phi_C^t) ) | |
7. |
If the first-order implicit Euler scheme is used, the value at t+ t/2 is replaced by the value at _________ |
A. | t |
B. | t- ( frac{ Delta t}{2} ) |
C. | t+ t |
D. | t- t |
Answer» D. t- t | |
8. |
Which of these changes should be made in the semi-discretized equation to get the fully discretized equation? |
A. | Express the face values in terms of the neighbouring face values |
B. | Express the face values in terms of the cell values |
C. | Express the cell values in terms of the face values |
D. | Express the cell values in terms of the neighbouring cell values |
Answer» C. Express the cell values in terms of the face values | |
9. |
Consider the following equation representing the temporal integration over the time interval t- ( frac{ Delta t}{2} ) and t+ ( frac{ Delta t}{2} ) at the spatial point C.
|
A. | If the first term is discretized using the difference of fluxes and the second term is evaluated using the midpoint rule, what is the discretized form? |
B. | (V_C ( rho_C phi_C)^{t- frac{ Delta t}{2}}+L( phi_C^t ) Delta t ) |
C. | (V_C ( rho_C phi_C)^{t+ frac{ Delta t}{2}}-L( phi_C^t ) Delta t ) |
D. | (V_C ( rho_C phi_C)^t+L( phi_C^t ) Delta t ) |
E. | (V_C ( rho_C phi_C)^{t+ frac{ Delta t}{2}}-V_C( rho_C phi_C)^{t- frac{ Delta t}{2}}+L( phi_C^t) Delta t ) |
Answer» E. (V_C ( rho_C phi_C)^{t+ frac{ Delta t}{2}}-V_C( rho_C phi_C)^{t- frac{ Delta t}{2}}+L( phi_C^t) Delta t ) | |
10. |
The discretization of the transient term using the finite volume approach is more like the spatial discretization of __________ |
A. | the convection term |
B. | the diffusion term |
C. | the source term |
D. | the anti-diffusion term |
Answer» B. the diffusion term | |