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6th class of Heat Transfer I
Thursday, January 30, 2014:
From textbook: J.P. Holman’s Heat
Transfer, 7th edition:
Fins (Section 2-10);
Thermal Contact Resistance
(Section 2-11)
Fins: Motorcycle Engine
Example Problem (fins): 2-67
Lcorrected = L + t/2 = 0.0064 m + 0.0016 m/2=
0.0072 m
r1 = 0.025 m /2 = 0.0125 m
r2c = r1 + Lc = 0.0125 m + 0.0072 m = 0.0197 m
r2c / r1 = 0.0197 m/ 0.0125 m = 1.5760
Am = t (r2c - r1 )= (0.0016 m)( 0.0197 m – 0.0125 m)
Am = 1.1520 x 10-5 m2
Lc
3/2 ( h/ (k Am ) ½ =
Example Problem (fins): 2-67
(concluded)
= (0.0072)3/2 (23/[(200)(1.1520 x 10-5 )])1/2 =
=0.0610
From Figure 2-12 in textbook: η = 98% = 0.98
qmaximum = 2π (r2c
2 – r1
2 ) h (To - T∞ )
= 2π [(0.0197)2 – (0.0125)2 ](23)(150 – 15)
= 4.5230 W
qactual = (4.5230 W)(0.98) = 4.4325 W
The heat lost by the fin is 4.43 Watts.
Example of Thermal Contact
Resistance (cylindrical electronic
component inside of heat sink)
Example Problem (thermal contact) 2-
9
Two 3.0 cm diameter 304 stainless-steel bars, 10
cm long, have ground surfaces and are exposed
to air with a surface roughness of about 1
micrometer. If the surfaces are pressed together
with a pressure of 50 atm and the two-bar
combination is exposed to an overall
temperature difference of 100 degrees Celsius,
calculate the axial heat flow and temperature
drop across the contact surface.
Solution Example Problem (thermal
contact) 2-9
See page 28, Equation 2-4: Heat flow = thermal
potential difference/thermal resistance, or
q = ∆Toverall /∑Rth
From page 34, Eqn. 2-12,
Rth= ∆x/kA (for conduction resistance), Rc =
1/hc A (for the contact resistance)
but there are three resistances in this system: one
conduction resistance in each bar, and one contact
resistance (between the two bars)
Solution Example Problem (thermal
contact) 2-9, continued
For the bars: Rth= ∆x/kA = (10 cm)(1m/100
cm)/(16.3 W/m•°C)(π((3.0 cm/2)(1m/100 cm))2 )=
8.679 °C/W.
The contact resistance: Rc = 1/hc A =
(5.28 (10-4 ) m2 ∙ °C/W)/(π((3.0 cm/2)(1m/100 cm))2
= 0.747 °C/W.
The total thermal resistance is then:
∑Rth = (2)8.679+0.747 = 18.105 °C/W.
Solution Example Problem (thermal
contact) 2-9, concluded
The overall heat flow is:
q = ∆Toverall /∑Rth = (100 deg C)/(18.105 deg C/W) =
5.52 W
The temperature drop across the contact surface
is: ∆Tc= (Rc /∑Rth ) ∆Toverall =
[(0.747 °C/W)/ (18.105 deg C/W )](100 deg C)
= 4.13 deg C
Questions?
References:
Slide 3: Retrieved on Sunday, August 27, 2017:
https://www.comsol.com/blogs/thermal-
contact-resistance-simulation/
Assignment: Read Sections 3-1, 3-2, and 3-3

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6th heat transfer class, thursday, january 30, 2014

  • 1. 6th class of Heat Transfer I Thursday, January 30, 2014: From textbook: J.P. Holman’s Heat Transfer, 7th edition: Fins (Section 2-10); Thermal Contact Resistance (Section 2-11)
  • 3. Example Problem (fins): 2-67 Lcorrected = L + t/2 = 0.0064 m + 0.0016 m/2= 0.0072 m r1 = 0.025 m /2 = 0.0125 m r2c = r1 + Lc = 0.0125 m + 0.0072 m = 0.0197 m r2c / r1 = 0.0197 m/ 0.0125 m = 1.5760 Am = t (r2c - r1 )= (0.0016 m)( 0.0197 m – 0.0125 m) Am = 1.1520 x 10-5 m2 Lc 3/2 ( h/ (k Am ) ½ =
  • 4. Example Problem (fins): 2-67 (concluded) = (0.0072)3/2 (23/[(200)(1.1520 x 10-5 )])1/2 = =0.0610 From Figure 2-12 in textbook: η = 98% = 0.98 qmaximum = 2π (r2c 2 – r1 2 ) h (To - T∞ ) = 2π [(0.0197)2 – (0.0125)2 ](23)(150 – 15) = 4.5230 W qactual = (4.5230 W)(0.98) = 4.4325 W The heat lost by the fin is 4.43 Watts.
  • 5. Example of Thermal Contact Resistance (cylindrical electronic component inside of heat sink)
  • 6. Example Problem (thermal contact) 2- 9 Two 3.0 cm diameter 304 stainless-steel bars, 10 cm long, have ground surfaces and are exposed to air with a surface roughness of about 1 micrometer. If the surfaces are pressed together with a pressure of 50 atm and the two-bar combination is exposed to an overall temperature difference of 100 degrees Celsius, calculate the axial heat flow and temperature drop across the contact surface.
  • 7. Solution Example Problem (thermal contact) 2-9 See page 28, Equation 2-4: Heat flow = thermal potential difference/thermal resistance, or q = ∆Toverall /∑Rth From page 34, Eqn. 2-12, Rth= ∆x/kA (for conduction resistance), Rc = 1/hc A (for the contact resistance) but there are three resistances in this system: one conduction resistance in each bar, and one contact resistance (between the two bars)
  • 8. Solution Example Problem (thermal contact) 2-9, continued For the bars: Rth= ∆x/kA = (10 cm)(1m/100 cm)/(16.3 W/m•°C)(π((3.0 cm/2)(1m/100 cm))2 )= 8.679 °C/W. The contact resistance: Rc = 1/hc A = (5.28 (10-4 ) m2 ∙ °C/W)/(π((3.0 cm/2)(1m/100 cm))2 = 0.747 °C/W. The total thermal resistance is then: ∑Rth = (2)8.679+0.747 = 18.105 °C/W.
  • 9. Solution Example Problem (thermal contact) 2-9, concluded The overall heat flow is: q = ∆Toverall /∑Rth = (100 deg C)/(18.105 deg C/W) = 5.52 W The temperature drop across the contact surface is: ∆Tc= (Rc /∑Rth ) ∆Toverall = [(0.747 °C/W)/ (18.105 deg C/W )](100 deg C) = 4.13 deg C
  • 10. Questions? References: Slide 3: Retrieved on Sunday, August 27, 2017: https://www.comsol.com/blogs/thermal- contact-resistance-simulation/ Assignment: Read Sections 3-1, 3-2, and 3-3