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Problem sets are preferably transmitted as e-mail attachments, alternatively placed in the instructors Perkins Hall 305 mailbox.
The homework archive is available for reference by registered students.
PE assignments submitted after the archive is opened will not be considered.
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(1) - Courseware |
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(2) - The Computational
Fluid-Thermal Sciences (AJB, 2009) |
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(3) - Fluid
Dynamics Handbook (AJB, 1998, Ch. 28) |
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(4) - The Computational Engineering Sciences (AJB, 2006) |
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Due Class |
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1.1
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Solve the steady viscous laminar-thermal
incompressible non-D !! Navier-Stokes equations for 2-D fully developed non-isothermal flow between horizontal parallel plates with plate fixed temperatures T1 and T2 > T1. Assume the viscous dissipation term in DE is negligible.
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2.1
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(2, Ch. 2) 4.1, 4.2, 4.3, 4.4
(optional)
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.2
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(2, Ch. 2) 5.1, 5.2
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6
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3.1
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(2, Ch. 2) 6.1, 6.2, 6.3
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.2
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(2, Ch. 2) 7.1, 7.2
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.3
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(2, Ch. 2) 8.1, 8.2, 8.3
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.4
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(2, Ch. 2) 10.1, 10.2
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.5
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(2, Ch. 2) 11.1, 11.2, 11.3
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.6
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(2, Ch. 3) 4.1, 5.1, 5.2, 5.3
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8
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4.1
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(2, Ch. 4) 2.1
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.2
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(2, Ch. 4) 3.1, 3.2
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.3
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(2, Ch. 4) 4.1, 4.2, 4.3
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.4
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(2, Ch. 4) 5.1
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10
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5.1
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(2, Ch. 4) 9.1, 9.2
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.2
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(2, Ch. 4) 9.3, 9.4, 9.5
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.3
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(2, Ch. 4) 10.1, 10.2, 10.3, 10.4
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.4
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(2, Ch. 4) 12.1, 12.3
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14
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6.1
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(2, Ch. 5) 2.1, 2.2, 2.3, 2.4
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.2
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(2, Ch. 5) 3.1
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.3
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(1; 4, Ch. CMn) Proceed through the Taylor
series process, page SVNS.3, to verify the vorticity Robin BC, egn. (CMn.49) Then
confirm the lower order forms in (4, Ch. CMn) eqn. (C,m/50),(CMn.51).
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.4
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(1) verify the details of the
GWSh template for {FQ}, page SVNS.5.
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.5
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(1) Confirm the {N1(z)}
basis convection term hyper-matrix, page SVNS.5A.
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.6
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(1) Detail the templates for GWSh
Newton jacobian, starting with the essence on page SVNS.6.
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.7
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(1) For the Taylor weak
statement omega-psi INS algorithm, verify the TS development leading to
the Beta term, page SVNS.12.
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.8
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(1) Examine the TWS aPSE
quasi-Newton template for the coupled fluid-thermal problem statement, hence confirm the formulation correctness.
Then copy and edit the quasi-Newton template to make it a Newton template
for this problem statement.
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18
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7.0
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For the pressure projection INS algorithm:
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.1
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(1; 2, Ch. 5) 4.1, 4.2, 4.3
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.2
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(1) Review, hence confirm the
PPNS algorithm key formulation, iteration and IC strategies detailed on
page PPNS.10.
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.3
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(1) Verify the correctness of
the PPNS template essence summarized on pages PPNS.12-13.
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.4
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(1) Convince yourself of the
correctness of the tensor product quasi-Newton jacobian, page PPNS.14,
focusing in particular on the role of the metric data strings in formation
of the convection term contributions.
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.5
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(1) For the TWSh
generalization to PPNS for error identification, confirm the TS operations
leading to Lm(q), page PPNS.16.
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.6
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(1) Confirm the matrix
expression for [AjAk], page PPNS.17, hence the
divergence form at the bottom of the page.
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.7
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(1) For the TKE closure model,
confirm the law-of-the-wall BC expressions, page PPNS.28.
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8.0
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For free-surface flow INS algorithms:
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.1
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(1) Confirm that DPz
ordering produces the form presented on page FSNS.1.
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.2
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(1) Verify that
DM is ill-posed as
an ODE expression for vertical velocity, page FSNS.2.
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.3
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(1) Confirm the non-D
depth-averaged flow PDE system, page FSNS.5, hence the hyperbolic
conservation law form, page FSNS.7.
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.4
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(1) Verify the flux vector
jacobian operations, page FSNS.9.
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.5
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(1) Convince yourself of the
accuarcy of the TWSh
+ TS template for depth-averaged INS, pages FSNS.10-11.
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.6
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(1) Review, hence confirm the
aPSE template for unsteady, turbulent depth-averaged INS, c.f., page
FSNS.15 for summary.
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26
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9.0
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For the computational spectral
theory:
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.1
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(2. Ch. 5) 6.1, 6.2
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.2
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(2. Ch. 5) 6.3, 6.4
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.3
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(2. Ch. 5) 6.5, 6.6
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.4
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(2. Ch. 5) 6.7, 6.8, 6.9
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.5
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(2. Ch. 5) 9.2, 9.3, 9.4
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TOP
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