Chapter 5 Numerical Method in Heat Conduction Flashcards

1
Q

What is the limitation of analytical methods

A

highly simplified problems in simple geometries or problems than can be simplified with reasomable approximations

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2
Q

Issues with the numerical method

A

only get numbers dont have neat solution -> plotting data without understanding physics

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3
Q

Numerical method adv

A

often oversimplify analytical soltuion to allow easier maths -> remove non linearity, therefore mathematical model more likely to be accurate
Allows quick iterations to check if variables chosen are correct and their impact
analytical solution may result in problem so complex not worth the effort to try and solve

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4
Q

what is m in numerical method

A

m is the number of points on the mesh

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5
Q

what do you want to happen to m to maximise accuracy

A

m-> infinity such that delta x tends to zero

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6
Q

Difference between the finite difference equation and the differential equation

A

differential equation is valid at every point whereas the finite difference equation is valid onoly at discrete points (the nodes)

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7
Q

What is the energy balance method

A

subdividing the medium into a sufficient number of volume elements and then applying an energy balance on each element

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8
Q

what is the energy balance in the energy balance method

A

rate of heat conduction at the left surface + rate of heat conduction at the right surface + rate of heat generation inside the element = rate of change of the energy content of the element

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9
Q

Energy balance in energy balance method =

A

Q.cond left + Q.con right + E.gen element = delta E element/ delta t

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10
Q

what is the change in energy content of an element equal to

A

zero

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11
Q

what is the numerical equivalent of a first order differential

A

Tm-1 - Tm / delta x

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12
Q

what is the numerical equivalent of a second order differential

A

Tm-1 - 2Tm + Tm+1 / delta x ^2`

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13
Q

What is assumed to happen between nodes in the finite difference formulation

A

variation is linear between nodes

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14
Q

What are the boundary conditions most commonly encountered in pracice

A

specified temperature, specified heat flux, convection and radiation

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15
Q

How is specified temperature dealt with

A
T(0)  = To = Specified value
T(L) = Tm = Specified value
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16
Q

What type of boundary conditions are dealt with using an energy balance on the volume element at the boundary

A

specified heat flux, convection, radiation or combined convection and radiation

17
Q

Equation for energy balance of volume element at boundary

A

Sum of Q. + E.gen element = 0

18
Q

Specified heat flux boundary condition

A

q.o * A + kA(T1-T0)/delta x + e.gen (Adelta x/2)

19
Q

If a surface is adiabatic how is boundary condition resolved

A

treat as symmetry line, temperature gradient slop is zero and if at T0, T1 and T-1 will be equal

20
Q

How many equations will you end up with

A

m equations

21
Q

how will the equations be computed

A

in a massive matrix of the form Ax = B or for our case AT=B
Where A is a matrix of known coefficients,
T is a matrix of unknown temperatures
and B a matrix of heat generation + other known stuff

22
Q

When resolving a boundary condition what will remain no matter what

A

at boundaries the conduction term on the other side of the element and the energy generation term inside the element, will the just ad additional terms for radiation, convection etc, internal will have the second derivative and energy generation terms

23
Q

What is an interface boundary condition

A

Two different solid media are assumed to be in perfect contact, thus at the same temperature interface node, but the rate of heat transfer via convection will be different due to different, convection coefficients

24
Q

What is the mirror image approach

A

can be used for problems that possess thermal symmetry, replace the plane of symmetry by insulation and only consider only half the medium in the solution -

25
Q

What does the finite difference formulation of steady heat conduction problems usually result in

A

a system of m algebraic equation in m unknown nodal temperatures that need to be solved simultaneously

26
Q

Two types of method for solving many simultaneous equations

A

direct and iterative

27
Q

Whats the difference between a direct and iterative method

A

direct methods are based on a fixed number of well defined steps that results in solution in a systematic manner, iterative methods are based on an initial guess for the solution that is refined by iteration until a specified convergence criterion is reached

28
Q

Give an example of direct approach

A

finding the inverse of the A matrix and solving A-1*b =T

do not use this approach in exams

29
Q

What is the gauss seidal method

A

iterative method, have equations relating all the temperatures, make initial guess and sub into equations, everytime you solve one update previous results