ME 410/1&2 – Heat Transfer

   Fall 2003

Solutions of HW # (4a) & (4b)

(Chapter 4: TRANSIENT HEAT CONDUCTION)

 

HW # (4a)

 


Lumped System Analysis

 

 


4-2C The lumped system analysis is more likely to be applicable for the body cooled naturally since the Biot number is proportional to the convection heat transfer coefficient, which is proportional to the air velocity. Therefore, the Biot number is more likely to be less than 0.1 for the case of natural convection.

 


4-6C Biot number represents the ratio of conduction resistance within the body to convection resistance at the surface of the body. The Biot number is more likely to be larger for poorly conducting solids since such bodies have larger resistances against heat conduction.

 

 


4-8C The cylinder will cool faster than the sphere since heat transfer rate is proportional to the surface area, and the sphere has the smallest area for a given volume.

 

 


4-14 The temperature of a gas stream is to be measured by a thermocouple. The time it takes to register 99 percent of the initial DT is to be determined.

Assumptions 1 The junction is spherical in shape with a diameter of D = 0.0012 m. 2 The thermal properties of the junction are constant. 3 The heat transfer coefficient is constant and uniform over the entire surface. 4 Radiation effects are negligible. 5 The Biot number is Bi < 0.1 so that the lumped system analysis is applicable (this assumption will be verified).

Properties The properties of the junction are given to be , , and .

Analysis The characteristic length of the junction and the Biot number are

               

Since , the lumped system analysis is applicable. Then the time period for the thermocouple to read 99% of the initial temperature difference is determined from

               


4-23 A number of carbon steel balls are to be annealed by heating them first and then allowing them to cool slowly in ambient air at a specified rate. The time of annealing and the total rate of heat transfer from the balls to the ambient air are to be determined.

Assumptions 1 The balls are spherical in shape with a radius of r0 = 4 mm. 2 The thermal properties of the balls are constant. 3 The heat transfer coefficient is constant and uniform over the entire surface.  4 The Biot number is Bi < 0.1 so that the lumped system analysis is applicable (this assumption will be verified).

Properties The thermal conductivity, density, and specific heat of the balls are given to be k = 54 W/m.°C, r = 7833 kg/m3, and Cp = 0.465 kJ/kg.°C.

Analysis  The characteristic length of the balls and the Biot number are

 

Therefore, the lumped system analysis is applicable. Then the time for the annealing process is determined to be

               

The amount of heat transfer from a single ball is

               

Then the total rate of heat transfer from the balls to the ambient air becomes   

               

 

 


4-24

"!PROBLEM 4-24"

 

"GIVEN"

D=0.008 "[m]"

"T_i=900 [C], parameter to be varied"

T_f=100 "[C]"

T_infinity=35 "[C]"

h=75 "[W/m^2-C]"

n_dot_ball=2500 "[1/h]"

 

"PROPERTIES"

rho=7833 "[kg/m^3]"

k=54 "[W/m-C]"

C_p=465 "[J/kg-C]"

alpha=1.474E-6 "[m^2/s]"

 

"ANALYSIS"

A=pi*D^2

V=pi*D^3/6

L_c=V/A

Bi=(h*L_c)/k "if Bi < 0.1, the lumped sytem analysis is applicable"

b=(h*A)/(rho*C_p*V)

(T_f-T_infinity)/(T_i-T_infinity)=exp(-b*time)

m=rho*V

Q=m*C_p*(T_i-T_f)

Q_dot=n_dot_ball*Q*Convert(J/h, W)

 

 

 

 

Ti [C]

time [s]

Q [W]

500

127.4

271.2

550

134

305.1

600

140

339

650

145.5

372.9

700

150.6

406.9

750

155.3

440.8

800

159.6

474.7

850

163.7

508.6

900

167.6

542.5

950

171.2

576.4

1000

174.7

610.3

 

 

 

 


 


4-29C The Fourier number is a measure of heat conducted through a body relative to the heat stored. Thus a large value of Fourier number indicates faster propagation of heat through body. Since Fourier number is proportional to time, doubling the time will also double the Fourier number.

 


4-30C This case can be handled by setting the heat transfer coefficient h to infinity  since the temperature of the surrounding medium in this case becomes equivalent to the surface temperature. 

 

 

 


4-36 Large brass plates are heated in an oven. The surface temperature of the plates leaving the oven is to be determined.

Assumptions 1 Heat conduction in the plate is one-dimensional since the plate is large relative to its thickness and there is thermal symmetry about the center plane. 3 The thermal properties of the plate are constant. 4 The heat transfer coefficient is constant and uniform over the entire surface.  5 The Fourier number is t > 0.2 so that the one-term approximate solutions (or the transient temperature charts) are applicable (this assumption will be verified).

Furnace,

700°C

 
Properties The properties of brass at room temperature are given to be k = 110 W/m.°C, a = 33.9´10-6 m2/s

Analysis The Biot number for this process is

           

The constants corresponding to this Biot number are, from Table 4-1,

             

The Fourier number is

           

Therefore, the one-term approximate solution (or the transient temperature charts) is applicable. Then the temperature at the surface of the plates becomes

           

 

Discussion This problem can be solved easily using the lumped system analysis since Bi < 0.1, and thus the lumped system analysis is applicable. It gives

which is almost identical to the result obtained above.

 


4-37  "!PROBLEM 4-37"

 

"GIVEN"

L=0.03/2 "[m]"

T_i=25 "[C]"

T_infinity=700 "[C], parameter to be varied"

time=10 "[min], parameter to be varied"

h=80 "[W/m^2-C]"

 

"PROPERTIES"

k=110 "[W/m-C]"

alpha=33.9E-6 "[m^2/s]"

 

"ANALYSIS"

Bi=(h*L)/k

"From Table 4-1, corresponding to this Bi number, we read"

lambda_1=0.1039

A_1=1.0018

tau=(alpha*time*Convert(min, s))/L^2

(T_L-T_infinity)/(T_i-T_infinity)=A_1*exp(-lambda_1^2*tau)*Cos(lambda_1*L/L)

 

T¥ [C]

TL [C]

500

321.6

525

337.2

550

352.9

575

368.5

600

384.1

625

399.7

650

415.3

675

430.9

700

446.5

725

462.1

750

477.8

775

493.4

800

509

825

524.6

850

540.2

875

555.8

900

571.4

 

 

 

time [min]

TL [C]

2

146.7

4

244.8

6

325.5

8

391.9

10

446.5

12

491.5

14

528.5

16

558.9

18

583.9

20

604.5

22

621.4

24

635.4

26

646.8

28

656.2

30

664

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 


4-40E Long cylindrical steel rods are heat-treated in an oven. Their centerline temperature when they leave the oven is to be determined.

Assumptions 1 Heat conduction in the rods is one-dimensional since the rods are long and they have thermal symmetry about the center line. 2 The thermal properties of the rod are constant. 3 The heat transfer coefficient is constant and uniform over the entire surface. 4 The Fourier number is t > 0.2 so that the one-term approximate solutions (or the transient temperature charts) are applicable (this assumption will be verified).

Properties The properties of AISI stainless steel rods are given to be k = 7.74 Btu/h.ft.°F, a = 0.135 ft2/h.

Analysis  The time the steel rods stays in the oven can be determined from