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Heat Transfer from Fins(Chapter 3)Zan Wu [email protected] Room: 5123
Fins
Fins/Extended surfaces
Why not called as convectors?
Radiators
Fins
Fan cooling is not sufficient for advanced microprocessors
Microfins
Microfin copper tube
Carbon nanotube microfinson a chip surface
Fin analysis
Two basic questionsØ What is the rate of heat dissipated by the fin?Ø What is the variation in the fin temperature from
the fin base to the fin tip?
Rectangular fin
2
2 0 (3 31)d Cdx Aϑ α
ϑλ
− = −
x dx
L
t1
Q1
.
tfb Z
Energy balance on the element from x to x + dx
A: area of a cross section normal to xC: perimeter of this section
)tt( f−=ϑSteady state1D
Cont’d
Boundary conditions:
Assume a long and thin fin, the heat transferred at the fin tip is negligible
)313(0AC
dxd2
2−=ϑ
λα
−ϑ
b2
bZZ2
ACm2
λα
=λ⋅α
≈λα
=
)tt(dxdt:Lx fLx −αʹ=λ−= =
0dxdt
Lx=⎟
⎠⎞
⎜⎝⎛
=
f111 tttt:0x −=ϑ=ϑ⇒==
x dx
L
t1
Q1
.
tfb Z
Rectangular fin
Solution:
cosh2
sinh2
mx mx
mx mx
e emx
e emx
−
−
+=
−=
1 2
3 4cosh sinh
mx mxC e C e
C mx C mx
ϑ −= + =
= +
Hyperbolic functions
At x = L ϑ = ϑ2
1 1
cosh ( ) (3 38)cosh
f
f
t t m L xt t mL
ϑϑ
− −= = −
−
2
1
1coshmL
ϑϑ
=
heat transfer from the fin?Q&
1 10
sinh ( )coshx
d mLQ A A mdx mL
CmA
ϑλ λ ϑ
αλ
=
⎛ ⎞= − = − ⋅ ⋅ −⎜ ⎟⎝ ⎠
= ⇒
&
1 1 1tanh 2 tanh (3 40)Q C A mL b Z mLα λ ϑ α λ ϑ= ⋅ = −g
Rectangular fin
Rectangular fin
α = 25 W/m2K, b = 2 cm, L = 10 cm
Rectangular fin
If the condition below is used, i.e., to consider heat loss from the fin tip
one has
and
and
LxLxdx
d=
=ϑαʹ=⎟
⎠⎞
⎜⎝⎛ ϑλ−
)413(mLsinh
mmLcosh
)xL(msinhm
)xL(mcosh
1−
λαʹ
+
−λαʹ
+−=
ϑϑ
)423(mLsinh
mmLcosh
11
2 −
λαʹ
+=
ϑϑ
)433(mLtanh
m1
mLtanhmAmQ 11 −
λαʹ
+
+λαʹ
ϑλ=!
Fins on Stegosaurus
Those plates absorb radiation from the sun or cool the blood?
Practical considerations
e.g.,Ø How to choose a fin material?ØHow to optimize fins?
Criterion for benefit
Fig. 3-13. Arrangement of rectangular fins
1
preferable if
0dQdL
>&
1 ( )Q function L=&L
.
Z
t1
b
1Q!
Fin effectiveness, fin efficiency
1
1
from the fin from the base area without the fin
η =&
&
1
1
from the finfrom a similar fin but with λ
ϕ == ∞
&&
Criterion: maximum heat flow at a given mass
M = ρ b L Z = ρ Z A1 A1 = b L, Z, ρ are given.
Find maximum for constant A1 = b⋅L.
C ≈ 2Z , A = b⋅Z
mLtanhACQ 11 ϑλα=!
b2
ACm2
λα
=λα
=
1Q!
!⎟⎠
⎞⎜⎝
⎛⋅
λα
⋅ϑ⋅αλ=bA
b2tanhZb2Q 1
11!
L
Zb
Optimal rectangular fin
Cont’d
Condition
1 0 gives optimum
after some algebra one obtains
21.419 (3 55)/ 2
dQdb
Lb b
λα
=
= −
&
M
Fin material selection
After some algebra one finds:
)523(bA
b2tanhZb2
mLtanhAmQ
11
11
−⎟⎠
⎞⎜⎝
⎛λα
ϑαλ=
=ϑλ=!
12 1.419Aub bαλ
= ⋅ =
1from the condition / 0dQ db =&
)a613(41
utanhu
Z1QA 233
3
1
11 −
λα⋅⎟⎟
⎠
⎞⎜⎜⎝
⎛
ϑ=!
For an optimized rectangular fin
Cont’d
M = ρ b L Z = ρ Z A1 =
ρ/λ is the material parameter see Table 3-1.
Aluminum instead of Copper. ρ/λ Aluminum: 11.8; Copper: 23.0
Why not Magnesium? ρ/λ Magnesium: 10.2
λρ⋅
α⋅⎟⎟
⎠
⎞⎜⎜⎝
⎛
ϑ= 232
3
1
1
41
utanhu
Z1Q!
Straight triangular fin
ϑ = t − tf
Heat balance ⇒
Solution:
K0 → ∞ as x → 0 ⇒ B = 0 because ϑ is finite for x = 0
x = L and ϑ = ϑ1 ⇒
)623(0bL2
x1
dxdx1
dxd2
2−=ϑ
λα
−ϑ
+ϑ
bL2
λα
=β
( ) )x2(BKx2AI 00 β+β=ϑ
( )L2AI01 β=ϑ
LxbZA ⋅=
δ
L
dx
x
b t1
tf1Q!
Bessel differential equation
I0 and K0 are the modified Bessel functions of order zero
Triangular fin
⇒
! )L2(IA
0
1β
ϑ=
)653()L2(I)x2(I
0
0
1−
β
β=
ϑϑ
Lx1 dx
dtAQ=⎭
⎬⎫
⎩⎨⎧ λ−=!!
)663()L2(I)L2(Ib2ZQ
0
111 −
ββ
αλϑ=⇒ !
Table 3.2 for numerical values of Bessel functions
Recap)383(
mLcosh)xL(mcosh
ft1tftt
1−
−=
−−
=ϑϑ
b22mλα
=
)403(mLtanh1Zb21Q −ϑαλ=!
mLtanhb2αλ
=η
mLmLtanh
=ϕ
21.419 (3 55)/ 2Lb b
λα
= −
)653()L2(0I)x2(0I
1−
ββ
=ϑϑ
bL2
λα
=β
11 1
0
(2 )2 (3-66)(2 )I LQ b ZI L
βαλ ϑ
β= ⋅ ⋅&
)L2(0I)L2(1I
b2
ββ
⋅αλ
=η
L)L2(0I/)L2(1I
βββ
=ϕ
21.309 (3 67)/ 2Lb b
λα
= −
Optimal fin: Maximum heat transfer at fixed fin mass
mL = 1.419 mL = 1.309
24
Circular or annular fins
Heat conducting area
A = 2πr b
Convective perimeter
C = 2 ⋅ 2πr = 4πr
r1 r2
b
How to calculate A and C for circular rod fins?
Fin efficiency for circular fins
How to use the fin efficiency in engineering calculations
s
flänsarareaoflänsad
QQQ
QQQ
finareaunfinned!!!
!!!
+=
+=
{( )
( )
fins b f
b b f fins
A t t
Q A t t Qλ
α
α ϕ=∞
−
= − + ⋅& &!
{ }( ) (3 71)b f b finsQ t t A Aα ϕ= − + ⋅ −&
Graphene
Anisotropic