HEAT TRANSFER :
STEADY STATE HEAT CONDUCTION
Prof. Pramod Maurya AP, SCOE, KHARGHAR 1
1. GENERAL HEAT CONDUCTION EQUATION : Rectangular Coordinates
2. GENERAL HEAT CONDUCTION EQUATION : Cylindrical and
Spherical Coordinates
3. BOUNDARY AND INITIAL CONDITIONS
4. STEADY HEAT CONDUCTION IN PLANE WALLS
5. The Thermal Resistance Concept
6. THERMAL CONTACT RESISTANCE
7. GENERALIZED THERMAL RESISTANCE NETWORKS
8. HEAT CONDUCTION IN CYLINDERS & SPHERES
9. CRITICAL RADIUS OF INSULATION
Prof. Pramod Maurya AP, SCOE, KHARGHAR 2
1. GENERAL HEAT CONDUCTION EQUATION : Rectangular Coordinates
Prof. Pramod Maurya AP, SCOE, KHARGHAR 3
Contd….
Prof. Pramod Maurya AP, SCOE, KHARGHAR 4
---------- Fourier-Biot equation
Contd….
Prof. Pramod Maurya AP, SCOE, KHARGHAR 5
2. GENERAL HEAT CONDUCTION EQUATION : Cylindrical Coordinates
GENERAL HEAT CONDUCTION EQUATION : Spherical Coordinates
Prof. Pramod Maurya AP, SCOE, KHARGHAR
3. BOUNDARY AND INITIAL CONDITIONS
6
• The mathematical expressions of the thermal conditions at the boundaries are called
the boundary conditions.
• The temperature at any
point on the wall at a
specified time also depends
on the condition of the wall
at the beginning of the heat
conduction process. Such a
condition, which is usually
specified at time t = 0, is
called the initial condition.
Prof. Pramod Maurya AP, SCOE, KHARGHAR
4. STEADY HEAT CONDUCTION IN PLANE WALLS
7
The energy balance for the wall can be
expressed as
Separating the variables in the above equation
and integrating
from x = 0, where T(0) = T1,
to x = L, where T(L) = T2, we get
Prof. Pramod Maurya AP, SCOE, KHARGHAR
5. The Thermal Resistance Concept
8
The heat conduction through a plane wall
can be rearranged as
a. Thermal circuit diagram for Conduction only b. Thermal circuit diagram for Convection only
Prof. Pramod Maurya AP, SCOE, KHARGHAR 9
c. The thermal resistance network for heat transfer through a plane wall subjected to
convection on both sides
where U is the overall heat transfer coefficient
Prof. Pramod Maurya AP, SCOE, KHARGHAR 10
d. Multilayer Plane Walls
Prof. Pramod Maurya AP, SCOE, KHARGHAR
6. THERMAL CONTACT RESISTANCE
11
• In reality, a surface is microscopically rough
no matter how smooth it appears to be.
• An interface contain numerous air gaps of
varying sizes that act as insulation because of
the low thermal conductivity of air
• Thus, an interface offers some resistance to
heat transfer, and this resistance per unit
interface area is called the thermal contact
resistance, Rc
Prof. Pramod Maurya AP, SCOE, KHARGHAR
7. GENERALIZED THERMAL RESISTANCE NETWORKS
12
a) Thermal resistance network for two
parallel layers
b) Thermal resistance network for combined
series-parallel arrangement
Prof. Pramod Maurya AP, SCOE, KHARGHAR
8. HEAT CONDUCTION IN CYLINDERS & SPHERES
13
A. cylindrical layer
Where, A = 2πrL
integrating
from r = r1, where T(r1) = T1,
to r = r2, where T(r2) = T2,
gives
Where
B. Spherical layer
Where
C. Cylindrical (or Spherical) shell subjected to
convection
Prof. Pramod Maurya AP, SCOE, KHARGHAR
CONTD…
14
C. Cylindrical (or Spherical) shell subjected to convection
for a cylindrical layer
for a spherical layer
Prof. Pramod Maurya AP, SCOE, KHARGHAR
CONTD…
15
D. Multilayered Cylinders and Spheres
The interface temperature T2 between the first and
second cylindrical layers can be determined from
Prof. Pramod Maurya AP, SCOE, KHARGHAR
8. CRITICAL RADIUS OF INSULATION
16
From thermal network, the
heat transfer rate :
differentiating above equation
with respect to r2 and equating
it to zero
A. For Cylinder
A. For Sphere
Prof. Pramod Maurya AP, SCOE, KHARGHAR 17

HEAT TRANSFER : STEADY STATE HEAT CONDUCTION

  • 1.
    HEAT TRANSFER : STEADYSTATE HEAT CONDUCTION Prof. Pramod Maurya AP, SCOE, KHARGHAR 1 1. GENERAL HEAT CONDUCTION EQUATION : Rectangular Coordinates 2. GENERAL HEAT CONDUCTION EQUATION : Cylindrical and Spherical Coordinates 3. BOUNDARY AND INITIAL CONDITIONS 4. STEADY HEAT CONDUCTION IN PLANE WALLS 5. The Thermal Resistance Concept 6. THERMAL CONTACT RESISTANCE 7. GENERALIZED THERMAL RESISTANCE NETWORKS 8. HEAT CONDUCTION IN CYLINDERS & SPHERES 9. CRITICAL RADIUS OF INSULATION
  • 2.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 2 1. GENERAL HEAT CONDUCTION EQUATION : Rectangular Coordinates
  • 3.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 3 Contd….
  • 4.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 4 ---------- Fourier-Biot equation Contd….
  • 5.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 5 2. GENERAL HEAT CONDUCTION EQUATION : Cylindrical Coordinates GENERAL HEAT CONDUCTION EQUATION : Spherical Coordinates
  • 6.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 3. BOUNDARY AND INITIAL CONDITIONS 6 • The mathematical expressions of the thermal conditions at the boundaries are called the boundary conditions. • The temperature at any point on the wall at a specified time also depends on the condition of the wall at the beginning of the heat conduction process. Such a condition, which is usually specified at time t = 0, is called the initial condition.
  • 7.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 4. STEADY HEAT CONDUCTION IN PLANE WALLS 7 The energy balance for the wall can be expressed as Separating the variables in the above equation and integrating from x = 0, where T(0) = T1, to x = L, where T(L) = T2, we get
  • 8.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 5. The Thermal Resistance Concept 8 The heat conduction through a plane wall can be rearranged as a. Thermal circuit diagram for Conduction only b. Thermal circuit diagram for Convection only
  • 9.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 9 c. The thermal resistance network for heat transfer through a plane wall subjected to convection on both sides where U is the overall heat transfer coefficient
  • 10.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 10 d. Multilayer Plane Walls
  • 11.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 6. THERMAL CONTACT RESISTANCE 11 • In reality, a surface is microscopically rough no matter how smooth it appears to be. • An interface contain numerous air gaps of varying sizes that act as insulation because of the low thermal conductivity of air • Thus, an interface offers some resistance to heat transfer, and this resistance per unit interface area is called the thermal contact resistance, Rc
  • 12.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 7. GENERALIZED THERMAL RESISTANCE NETWORKS 12 a) Thermal resistance network for two parallel layers b) Thermal resistance network for combined series-parallel arrangement
  • 13.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 8. HEAT CONDUCTION IN CYLINDERS & SPHERES 13 A. cylindrical layer Where, A = 2πrL integrating from r = r1, where T(r1) = T1, to r = r2, where T(r2) = T2, gives Where B. Spherical layer Where C. Cylindrical (or Spherical) shell subjected to convection
  • 14.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR CONTD… 14 C. Cylindrical (or Spherical) shell subjected to convection for a cylindrical layer for a spherical layer
  • 15.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR CONTD… 15 D. Multilayered Cylinders and Spheres The interface temperature T2 between the first and second cylindrical layers can be determined from
  • 16.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 8. CRITICAL RADIUS OF INSULATION 16 From thermal network, the heat transfer rate : differentiating above equation with respect to r2 and equating it to zero A. For Cylinder A. For Sphere
  • 17.
    Prof. Pramod MauryaAP, SCOE, KHARGHAR 17