Chapter 4 Transient Heat Conduction Flashcards

1
Q

What does lumped system analysis represent

A

when the interior temperature of a body remains essentially uniform at all times during heat transfer process

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2
Q

What does lumped system analysis allow

A

Temperature to be taken as a function of Time only T(t)

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3
Q

What could be represented as lumped system analysis

A

a small copper ball

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4
Q

What is the energy balance for a heated solid body (words)

A

heat transfer into the body during dt = the increase in the energy of the body during dt

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5
Q

Energy balance of a solid body =

A

hAs(Tinf - T) dt = mcp dT

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6
Q

Lumped system analysis equation

A

(T(t) - Tinf) / Ti - Tinf = e-^bt where b = hAs / rhoVcp

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7
Q

Proof of lumped system analysis equation

A

integrat energy balance equation between T(t) and Ti t=t and t=0

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8
Q

What does lumped system analysis assume

A

T is only dependent on time not on displacement

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9
Q

What happens as you increase b for lumped system analysis

A

the lumped system will reach the ambient temperature much quicker

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10
Q

How does the temperature of a lumped system analysis vary with time

A

Temperature changes dramatically initially before slowing down

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11
Q

What can be assumed about resistance for valid lumped system analysis

A

the resistance of conduction is much smaller than the resistance of convection -> convection is limiting factor heat is quickly distributed throughout system

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12
Q

For lumped system what is the rate of convection heat transfer between the body and its environment at time t

A

Q.(t) = hAs(T(t) - Tinf)

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13
Q

For lumped system what is the total amount of heat transfer between the body and the surrounding medium over the time interval t=0 to t

A

Q = mcp (T(t) - ti)

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14
Q

The total maximum amount of heat transfer between the body and its surrounding is

A

Qmax = mcp (Tinf - Ti)

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15
Q

When is lumped system analysis applicable

A

when Bi <= 0.1

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16
Q

What happens when Bi <= 0.1

A

the temperatures within the body relative to the surroundings remain within 5 percent of each other

17
Q

What is the characteristic length in the biot number defined as

A

Lc = V / As

18
Q

How is the biot number calculated

A

Bi = hLc /k

19
Q

What is the biot number

A

ratio of heat convection to heat conduction

20
Q

What is the biot number equal to

A

convection at the surface of the body/ conduction within the body, and
conduction resistance within the body / convection resistance within the body

21
Q

What are the criteria for satisfying lumped system analysis

A

Small Biot number there, small bodies with high thermal conductivity and low convection coefficients are best

22
Q

What happens when convection coefficient h is high and k is low

A

large temperature differences occur between the inner and outer regions of a large solid

23
Q

What is the differential equation that describes transient heat transfer

A

d^2 T/ dx^2 = 1/alpha * dT/dt

where alpha is thermal restivity k/rho*cp

24
Q

What are the boundary conditions for a large plane wall x =0 at the centre

A

symmetry line at the centre, therefore dT(0,t)/dx = 0

and at x = L at surface heat transfer to via conduction = heat transfer from via convection

25
Q

What is dimensionless temperature theta(x,t) =

A

(T(x,t) - Tinf)/(Ti - Tinf)

26
Q

What is dimensionless distance X =

A

x/L

27
Q

What is dimensionless time tau =

A

tau = alpha * t/L^2 = fourier number

28
Q

What is the dimensionless differential equation =

A

d^2 theta / dX = d theta / d tau

should be partial derivatives

29
Q

What is the dimensionless heat transfer coefficient

A

biot number = hL/k

30
Q

What are the dimensionless BCs and ICs of a large plane wall equal to

A
BCs dtheta(0, tau)/dX = 0 and d theta(1, tau)/ dX = -Bi*theta(1, tau)
ICs theta(X, 0) = 1
31
Q

Why do we nondimensionalise all these quantities

A

reduces the number of independent variables in one dimensionalised transient conduction problems from 8 to 3

32
Q

Instead of doing exact maths how do we approach transient heat transfer problems

A

use the graphs

33
Q

What is the physical significance of the fourier number

A

measure of heat conducted through a body relative to heat stored
a large value means fast propagation of heat through a body

34
Q

what is the ratio of the fourier number

A

rate at which the heat is conduced across L of a body of volume L^3, to the rate at which heat is stored in a body of volume L^3

35
Q

What is a semi infinite solid

A

an ideaised body that has a single plane surface that extends to infinity in all directions

36
Q

What ca the earth be considered as

A

a semi infinite medium in determine variation of temperature near its surface

37
Q

When can most bodies be modeled as semi infinite solids

A

for short periods of times since heat does not have sufficient time to penetrate deep into the body

38
Q

When can the similarity variable solution be used

A

when you have a constant temperature Ts on the surface of a semi infinite solid