1B Chapter1 Sec.1.3 Color
Transcript of 1B Chapter1 Sec.1.3 Color
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Relationship to Thermodynamics
Chapter One
Section 1.3
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Alternative Formulations
Alternative Formulations
Time Basis:
At an instant
or
Over a time interval
Type of System:
Control volume
Control surface
An important tool in heat transfer analysis, often
providing thebasis for determiningthe temperature
of a system.
CONSERVATION OF ENERGY
(FIRST LAW OF THERMODYNAMICS)
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At an Instant of Time:
Note representation of system by a
control surface (dashed line)at the boundaries.
Surface Phenomena
,
in out
: rate
energy transfer across the controlof thermal and/or mechanical
due to heat transfer, fluid flow and/or work interactions.surface
E E
Volumetric Phenomena
: rate of due to conversion from another energy form
(e.g., electrical, nuclear, or chemical); energy conversion proc
thermal ener
ess occurs w
gy generatio
ithin the sy e
n
m.
st
gE
stenergy: storate of rage inchang the se o ysf m.teE
Conserv
ation of Energy
in out stst
gdE
dtE E E E (1.12c)
Each term has units of J/s or W.
APPLICATION TO A CONTROL VOLUME
Over a Time Interval
Each term has units of J.
in out stgE E E E (1.12b)
CV at an Instant and over a Time Interval
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At an instant
tdUq Wdt
Special Cases (Linkages to Thermodynamics)
(i) TransientProcess for a Closed Systemof Mass (M) Assuming Heat Transfer
to the System (Inflow) and Work Done by the System (Outflow).
Over a time intervaltot
stQ EW (1.12a)
Closed System
For negligible changes in potential or kinetic energy
tQ W U
Internalthermal energy
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Example 1.4: Application to thermal response of a conductor with Ohmic
heating (generation):
Involves change in thermal energyand for an incompressible substance.
tdU dT
Mcdt dt
Heat transfer is from the conductor (negative )q
Generation may be viewed as electrical workdone on the system (negative )W
Example 1.4
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Example 1.6: Application to isothermal solid-liquid phase change in a container:
Latent Heat
of Fusion
latt sfU U Mh
Example 1.6
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(ii) Steady Statefor Flow through an Open Systemwithout Phase Change or
Generation:
flow ow rkpv enthalp ytu pv i
in out in out
ideal gas constant specific heFor an w :atith
pi i c T T
in out in out
in out
For an :incompressible liqu
0
id
u u c T T
pv pv
2 2
in
in
out0
2 2
0out
For systems with significant heat transfer:
V V
gz gz
At an Instant of Time:2
out
02t
m u pv V gz W
2
in2t
m u pv V gz q
(1.12d)
Open System
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Surface Energy Balance
A special case for which no volume or mass is encompassed by the control surface.
Conservation of Energy(Instant in Time):
outin 0E E (1.13)
Applies for steady-state and transient conditions.
Consider surface of wall with heat transfer by conduction, convection and radiation.
cond conv rad 0q q q
4 41 2 2 2 2 sur 0T T
k h T T T T L
With no mass and volume, energy storage and generation are not pertinent to the energy
balance, even if they occur in the medium bounded by the surface.
THE SURFACE ENERGY BALANCE
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Methodology
On a schematicof the system, represent the control surfaceby
dashed line(s).
Choose the appropriate time basis.
Identify relevant energytransport, generation and/or storage terms
by labeled arrowson the schematic.
Write the governing form of the Conservation of Energyrequirement.
Substitute appropriate expressions for terms of the energy equation.
Solve for the unknown quantity.
METHODOLOGY OF FIRST LAW ANALYSIS
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Problem 1.57: Thermal processing of silicon wafers in a two-zone furnace.
Determine (a) the initial rate of change of the wafer
temperature and (b) the steady-state temperature.
Problem: Silicon Wafer
KNOWN: Silicon wafer positioned in furnace with top and bottom surfaces exposed to hotand cool zones, respectively.
FIND: (a) Initial rate of change of the wafer temperature from a value of 300K,w,iT and (b)
steady-state temperature. Is convection significant? Sketch the variation of wafer temperature
with vertical distance.
SCHEMATIC:
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Problem: Silicon Wafer (cont.)
ASSUMPTIONS: (1) Wafer temperature is uniform, (2) Hot and cool zones have uniformtemperatures, (3) Radiation exchange is between small surface (wafer) and large enclosure
(chamber, hot or cold zone), and (4) Negligible heat losses from wafer to pin holder.
ANALYSIS: The energy balance on the wafer includes convection to the upper (u) and lower
(l) surfaces from the ambient gas, radiation exchange with the hot- and cool-zones and an energystorage term for the transient condition. Hence, from Eq. (1.12c),
in out stE E E
or, per unit surface area
rad, rad, cv, cv,w
h c u l d T
q q q q cd
dt
4 4 4 4sur,sur, ww c w u w l whd T
T T T T h T T h T T cd dt
(a) For the initial condition, the time rate of change of the wafer temperature is determined
using the foregoing energy balance with , 300K,w w iT T
8 2 4 4 4 8 2 4 4 4 440.65 5.67 10 W / m K 1500 300 K 0.65 5.67 10 W / m K 330 300 K
2 28W / m K 300 700 K 4W / m K 300 700 K
32700 kg / m 875J / kg K 0.00078 /w im dT dt
104 K/sw idT / dt