Thermodynamics Processor Cooler
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Transcript of Thermodynamics Processor Cooler
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8/20/2019 Thermodynamics Processor Cooler
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Thermodynamics Mini Project Date: 12 Apr 2014
A computer is kept on all the time to monitor financial stock exchanges. The core functions of
the computer are mainly carried out by its processor chip. The shape of the processor is like aflat slab ith dimensions of 10mm by !mm by "nm# as shon in $ig. 1 belo.
%ome of the electrical energy used by the processor is lost as heat# leading to heat generation
ithin the processor. The rate at hich heat is generated ithin the processor chip of the
computer is 0.04&. 'ence# there is a fan in the computer hich blos air past the processor
chip to cool it don.
a( )ne day# the fan of the computer malfunctioned and stopped orking. 'o long ill it
take for the computer to o*erheat and spoil+ Assume that the computer ill fail once the
processor chip reaches a temperature of 100,-.
b( &hat poer rating should the replacement fan be if e ant to keep the maximum
temperature of the processor chip at 0,-+
Assumptions:1. Temperature of air is constant at 2,-.
2. The processor chip is made of pure silicon.
/. )nly top side of the processor chip is exposed to air# as illustrated in $ig. 1.
4. A circular fan is used# and the diameter of the fan is /cm.
!. Density of air is constant.
Figure 1. Structure of the computer processor
a( The thermal conducti*ity# k# of %i is 1/0 &m. hile its thermal diffusi*ity# # is 310
!m2s.
The con*ecti*e heattransfer coefficient of air can be taken to be 10 &m 2.
5olume of the processor 6 710310/( 37!310/( 37"310"( 6 4.!3101/ m/
Area of the exposed surface 6 710310 /( 37!310/( 6 !310! m2
B i=hV kA = (10)(4.5×10
−13
)(130)(5×10−5)
=6.92×10−10≪0.1
%ince the 8i *alue is less than 0.1# e can treat this as a lumped parameter case.
Doing some energy balance# e get
q́−hA (T −T ∞ )= ρ C p V dT
dt
9et beT −T ∞
d θ
dT
= q́
ρ C p V
− h A
ρC p V
θ= ´ A−B́ θ
here
´ A= q́
ρ C p V and
B́= h A
ρC p V
10mm
5mm
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∫0
θ1
´ A−B́ θdθ=∫
0
t
dt t =−1B́
ln( ´ A− ́B θ´ A )´ A=
q́ ρ C p V
= q́k
α V
= 0.04
130
8×10−5 (4.5×10
−13
)
=54701
B́= h A
ρC p V =
h A
k
α V
= 10(5×10−5)130
8×10−5 (4.5×10
−13)=683.76
t = −1
683.76ln( 54701− (683.76 ) (100−28 )54701 )=3.37×10−3 s
b( To make sure -;< does not o*erheat# a *ertically orientated fan as considered forcooling the -;
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P=% ∆ p
$=
& D2
U ∞
4$∆ p=
& D2
U ∞
4$
0.664
# √ μρLU ∞
3=4 μ '
Figure 2. Raspberry pi micro fan (D1!mm". #t uses P$.$%&'.')'.2* and it is !'+'''times more
po,erfu- than the considered design in part (b"
9imitations to our calculations are due to our assumptions abo*e as ell as assuming that
heat loss is only due to con*ection. Cn reality# a microprocessor is made up of *arious other
materials and does not really ha*e a solid slab structure# and heat can be lost in any direction
and not restricted to con*ection.