Module 1. Conduction heat transfer
Lesson 3
PROBLEMS ON HEAT CONDUCTION THROUGH PLANE/COMPOSITE WALLS HAVING VARIABLE THERMAL CONDUCTIVITY
Q. 1: Determine the hourly loss of heat through a brick wall 5 m long, 3 m high and 250 mm thick. If wall surface temperature. t1=20°C and t2 = -30°C. The λbrick = 0.6 kcal/m-hr-°C.
Solution:
Conductivity, λ = 0.6 kcal/m-hr-°C.
Thickness, δ = 250 mm = 250 × 10-3 m = 0.25 m
q
= 120 [kcal/m2-hr]
q = loss of heat through 15 m2 area of brick = q x A = 120 x 15 = 1800 kcal/hr
Q = 1800 kcal/hr.
Q. 2: Determine 𝛌,
thermal conductivity of a wall if q = 100 kcal/m2-hr at thickness, 𝛅
=
30 mm and ∆t
= 30°C.
Solution:
Heat transferred, q = 100 kcal/m2-hr
Thickness, 𝛅 =30 mm = 30 x 10-3m
= 0.03 m
∆t = 30°C
𝛌 = 0.1 [kcal/m-hr-oC]
Q. 3: Determine the rate of heat flow through a flat fire clay wall 𝛅 = 0.5 m & also find true distribution of temperature. If t1 = 1000°C & t2 = 0°C, 𝛌 =1.0 x (1+0.001t).
Solution:
q = rate of heat flow, λm = mean conductivity, tm = mean temperature.
λm
= 1.0[1+0.001×500) = 1.5 [kcal/m-hr-oC]
For true distribution of temperature:
b = 0.001, t1 = 1000, x0 = 1.
Equations of the temperature curve at any location =
So, for
different values of x; x = 0, 0.1, 0.2, 0.3, 0.4, 0.5
x |
True distribution of temperature
|
Equation of temperature curve
|
0 0.1 0.2 0.3 0.4 0.5 |
1000 844 673.3 488.2 264.9 0 |
1000 800 600 400 200 0 |
Q. 4: Determine the quantity of heat passing per hour through 1 m2 area of a boiler wall, if it is 20 mm thick and the thermal conductivity of its material is 50 kcal/m-hr-°C. The inner surface of the wall is covered by a layer of scale of thickness 2 mm whose thermal conductivity is 1.0 kcal/m-hr-°C. The temperature of the outer surface is 250°C and of the inner surface is 200°C.
Solution:
Thermal
resistance =
δ = Thickness
λ = Thermal conductivity
Thermal
resistance of outer surface =
δ1, (Thickness)= 20 mm =
0.02 m
λ1, Thermal conductivity of outer Surface = 50 kcal/m-hr-°C
Thermal resistance of outer surface = 0.02/50 = 4x 10-4 [m2-hr-°C/kcal]
Thermal
resistance of inner surface =
δ2, Thickness
= 2 mm = 0.002 m
λ2, Thermal conductivity of inner surface = 1.0 kcal/m-hr-°C
Thermal
resistance of inner surface = = 0.002/1 = 20x 10-4 [m2-hr-°C/kcal]
Quantity of heat passing,
t1 = temperature of outer surface, t2 = temperature of inner surface
t2 = 250°C, t1 = 200°C
= 2.08 x 104 [kcal/m2-hr] = 20800 [kcal/m2-hr]
t = t1
– q =
Temperature of contact = 250-20,800 x 4x10-4
t = 241.7°C
Q. 5: The rate of heat flow (q) through a plane wall of thickness δ = 50 mm is70 watt/m2. Determine the difference between the temperatures of wall surfaces and the numerical values of the temperature gradient through the wall if it is made from
(a) Brass whose λ = 70 watt/m-°C
(b) If wall is made of red brick whose λ = 0.7 watt/m-°C
Solution:
Temperature gradient = ∆t/δ
q = Rate of heat flow
λ = Thermal conductivity
δ = Thickness
∆t = Difference between temperature of wall surfaces.
(a) Brass
q = 70 watt/m2
δ = 50 mm =
50 x 10-3 = .05 m
λ = for brass = 70 watt/m-°C
Temperature Gradient = 0.05/0.05 = 1°C/m
(b) For Red Brick
λ for red brick = 0.7 watt/m-°C
5°C = ∆t
Temperature Gradient = 5/0.05 = 100°C/m
(c) For cork
λ for cork = 0.07 watt/m-°C
∆t = 50C
Temperature Gradient = ∆t /δ = 50/0.05 = 1000°C/m
Q. 6: Determine the loss of heat Q (watts) through a wall laid of lead brick of length 5 m, height 4 m and thickness 0.25 m, if the temperature of the surfaces of the wall are maintained at 110°C & 40°C. Assume λbrick = 0.7 watt/m-°C.
Solution:
λ, thermal conductivity = 0.7 watt/m-°C
δ = thickness = 0.25 m
∆t,
temperature difference of surfaces = (110-40) = 70°C
= 196 watt/m2
Q, loss of heat through 20 m2 area of wall = q x A= 196 x 20 = 3920 watt
Q = 3920 watt
Q. 7: It is necessary to insulate a flat surface such that the loss of heat from unit area of this surface per unit time will not exceed 450 watt/m2. The temperature of the surface underneath the layer of insulation is the 450°C and the layer temperature of the external surface of the insulating layer is 50°C. Determine the thickness of insulation for the following two cases
(a) The insulation is made from sobelite for which, λ = [0.09 + 0.0000874 t] watt/m°C.
(b) The insulation is made from Asbestos cement for which λ = [0.09 + 0.000146 t] watt/m°C.
Solution,
Case a:
λ = [0.09 + 0.0000874 t] watt/m-°C
t = 50°C
λ1 = [0.09 + 0.0000874 x 50] = 0.09437 watt/m-°C.
t = 450°C
λ2
= [0.09+0.0000874×450] = 0.12933 watt/m-oC
q, loss of heat from surfaces = 450 watt/m2
∆t, Temperatures differences = (450-50) = 400°C
Δ = 100 mm
Case
b:
λ = [0.0109 + 0.000146t]
t = 50°C
λ1 = (0.109 + 0.000146 x 50) = 0.1163 watt/m-°C.
t = 450°C
λ2 = [0.109 + 0.000146 x
450] = 0.1747 watt/m-°C
q, loss of heat from surfaces = 450 watt/m2
∆t, Temperatures differences = (450 - 50) = 400°C
δ,
thickness of insulation = 129.3 mm