Lecture 3 - Lumped System Analysis (DOBSON) Flashcards

1
Q

What is lumped system analysis and why is it useful?

A

This approximation is useful to simplify otherwise complex differential heat equations. Reduces the thermal system to a no. of distinct regions. Assumes the temp difference inside each region is negligible.

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2
Q

Can you draw the graph of temp vs distance for brick-insulation-blocks as part of a wall? And also the flow diagram?

A

YES OR NO

T1 -> Fbr -> T2 -> Fi -> T3 -> Fbl -> T4

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3
Q

What would a better represntation of the temp variation in the wall system?

A

Temp variation within the discrete regions. DRAW GRAPH.

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4
Q

How can the maths of DC electrical conduction be applied to hear currents?

A

Thermal Resistances -> electrical resistances
Temperature -> voltage
Heat flux -> electrical current

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5
Q

Fouriers law?

A

q= kA dT/dx = dT/dx/kA

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6
Q

what does dx/kA represent?

A

A description of how well the particle conducts heat as a result of its size, shape and material therefore:
dx/kA = Rth and q = dT/Rth, which is equivalent to ohms law. (q= I, dT = V, Rth = R).

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7
Q

What are the assumptions and approximations of this method?

A

The individual discrete regions that the model has been simplified down to are homogeneous:
- complex materials (e.g. composites) need to be simplified to produce a single thermal resistance value.
- thermal variations within a single region are not considered.
It is assumed that the model is unchanging with time:
- this is due to the fact that, as a purely resistive model (no capacitance), no part of the model is capable of absorbing energy.
The approach can not be relied upon to model micro and nano scale thermal behaviour.

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8
Q

How can we consider conduction through a plane?

A

By integrating fourier’s law to give:- q= (-kA/deltax)(T2-T1)
q = heat transfer rate
delta x = thickness of plane
k = thermal conductivity
A = area of plane
T2 - T1 = thermal difference across the plane

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9
Q

Can you write the expression from conduction through a plane in a form analogous to an electrical circuit?

A

HEAT FLOW = THERMAL POTENTIAL DIFFERENCE / THERMAL RESISTANCE

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