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Announcement MATHCAD for solving system of equation for HW1b

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Presentation on theme: "Announcement MATHCAD for solving system of equation for HW1b"— Presentation transcript:

1 Announcement MATHCAD for solving system of equation for HW1b
Tomorrow 5:30 pm this studio (computer lab)

2 Lecture Objectives: Discuss HW1b
Answer your questions Analyze the unsteady-state heat transfer numerical calculation methods

3 Unsteady-state heat transfer (Explicit – Implicit methods)
Example: To - known and changes in time Tw - unknown Ti - unknown Ai=Ao=6 m2 (mcp)i=648 J/K (mcp)w=9720 J/K Initial conditions: To = Tw = Ti = 20oC Boundary conditions: hi=ho=1.5 W/m2 Tw Ti To Ao=Ai Conservation of energy: Time [h] 0.1 0.2 0.3 0.4 0.5 0.6 0.7 To 20 30 35 32 10 15 Time step Dt=0.1 hour = 360 s

4 Explicit – Implicit methods example
Conservation of energy equations: Wall: Air: After substitution: For which time step to solve: +  or  ? Wall: Air: +  Implicit method  Explicit method

5 Implicit methods - example
After rearranging: 2 Equations with 2 unknowns!  = To Tw Ti  =36 system of equation Tw Ti  =72 system of equation Tw Ti

6 Explicit methods - example
 =360 sec  = To Tw Ti  =360 To Tw Ti  =720 To Tw Ti Time There is NO system of equations! UNSTABILE

7 Problems with stability !!! Often requires very small time steps
Explicit method Problems with stability !!! Often requires very small time steps

8 Explicit methods - example
 = To Tw Ti  =36 To Tw Ti  =72 To Tw Ti Stable solution obtained by time step reduction 10 times smaller time step Time  =36 sec

9 Explicit methods information progressing during the calculation
Tw Ti To

10 Unsteady-state conduction - Wall
q Dx Nodes for numerical calculation

11 Discretization of a non-homogeneous wall structure
Section considered in the following discussion Discretization in space Discretization in time


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