- D27 Gfem Q1 The Heat Transfer In The Shown Bar Could Be Approximated By The Following Equation K Oz2 Q 0 Where T Is Th 1 (47.17 KiB) Viewed 12 times
d27 GFEM Q1: The heat transfer in the shown bar could be approximated by the following equation: k öz2+Q=0 Where T is th
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d27 GFEM Q1: The heat transfer in the shown bar could be approximated by the following equation: k öz2+Q=0 Where T is th
d27 GFEM Q1: The heat transfer in the shown bar could be approximated by the following equation: k öz2+Q=0 Where T is the temperature in Kelvin, k is the thermal conductivity of the bar material in W/(m.K). and Q is the internal heat generation rate in W/m! Using the Galerkin finite element method find the temperature distribution for the following boundary conditions: T(0)=273 K dT 1D Bar =0 dxlyet Take the bar length to be 1 m, and the internal heat generation rate as: Q = x Q2: The quasi 1-D incompressible flow in a nozzle is described by the following equation: an () = Where is the potential function, A(x) is the area of the nozzle and is given by: A(x) = 1 -0.2x OSXS1 Nozzle Using the Galerkin finite element method find the potential function distribution for the following boundary conditions: (0) = 0 and N- inlet BRY Quasy Flow 1-0 O d = 0.2 dxxsi Generic shape for a nozzle