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International Journal of Mathematics and Statistics Invention (IJMSI)
E-ISSN: 2321 – 4767 P-ISSN: 2321 - 4759
www.ijmsi.org Volume 1 Issue 2 ǁ December. 2013ǁ PP-56-63

Quasi Static Thermal Stresses in A Limiting Thick Circular Plate
with Internal Heat Generation Due To Axisymmetric Heat
Supply
C. M. Bhongade1 and M. H. Durge2
1

2

Department of Mathematics, Shri. Shivaji College,Rajura, Maharashtra, India
Department of Mathematics, Anand Niketan College, Warora, Maharashtra, India

ABSTRACT: The present paper deals with the determination of quasi static thermal stresses in a limiting thick
circular plate with internal heat generation subjected to axisymmetric arbitrary heat flux on upper and lower
surface and the fixed circular edge is thermally insulated. Initially the plate is at zero temperature. Here we
modify Kulkarni [1]and compute the effects of internal heat generation and axisymmetric heat supply in terms
of stresses along radial direction. The governing heat conduction equation has been solved by the method of
integral transform technique. The results are obtained in a series form in terms of Bessel’s functions. The results
for temperature change, displacement and stresses have been computed numerically and illustrated graphically.

KEYWORDS: Quasi static thermal stresses, limiting thick circular plate, internal heat generation,
axisymmetric heat supply.

I.

INTRODUCTION

During the last century the theory of elasticity has found of considerable applications in the solution of
engineering problems. Thermoelasticity contains the generalized theory of heat conductions, thermal stresses. A
considerable progress in the field of air-craft and machine structures, mainly with gas and steam turbines and the
emergence of new topics in chemical engineering have given rise to numerous problems in which thermal
stresses play an important role and frequently even a primary role. Nowacki [2] has determined the temperature
distribution on the upper face, with zero temperature on the lower face and the circular edge thermally insulated.
Bhongade and Durge [3] studied an inverse steady state thermal stresses in a limiting thick circular plate with
internal heat generation.
Most recently Bhongade and Durge [4] considered thick circular plate and discuss the effect of Michell
function on steady state behavior of thick circular plate, now here we consider a thick circular plate with
internal heat generation subjected to axisymmetric arbitrary heat flux on upper and lower surface and the fixed
circular edge is thermally insulated. Initially the plate is at zero temperature. Here we modify Kulkarni [1] and
compute the effects of internal heat generation and axisymmetric heat supply on the limiting thick circular plate
in terms of stresses along radial direction. The governing heat conduction equation has been solved by the
method of integral transform technique. The results are obtained in a series form in terms of Bessel’s functions.
The results for temperature change, displacement and stresses have been computed numerically and illustrated
graphically. A mathematical model has been constructed with the help of numerical illustration by considering
steel (0.5% carbon) limiting thick circular plate. No one previously studied such type of problem. This is new
contribution to the field.
The direct problem is very important in view of its relevance to various industrial mechanics subjected
to heating such as the main shaft of lathe, turbines and the role of rolling mill, base of furnace of boiler of a
thermal power plant and gas power plant.

II.

FORMULATION OF THE PROBLEM

Consider a limiting thick circular plate of radius a and thickness 2h defined by
Initially the plate is at zero temperature. Let the plate be subjected to a axisymmetric arbitrary heat flux
prescribed over the upper surface
and the lower surface
The fixed circular
edge
is thermally insulated. Assume a limiting thick circular plate with internal heat generation is free
from traction. Under these prescribed conditions, the quasi static transient thermal stresses are required to be
determined.
The differential equation governing the displacement potential function
is given in [5] as

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56 | P a g e
Quasi Static Thermal Stresses In A Limiting Thick…
(1)
where K is the restraint coefficient and temperature change
is initial temperature.
Displacement function is known as Goodier’s thermoelastic displacement potential.
The temperature of the plate at time t satisfying the heat conduction equation as follows,
(2)
with the boundary conditions
(3)
(4)
(5)
and the initial condition
at
(6)
where is the thermal diffusivity of the material of the plate, k is the thermal conductivity of the material of
the plate, q is the internal heat generation and
is well known dirac delta function of argument r.
The Michell’s function M must satisfy
(7)
where
(8)
The components of the stresses are represented by the thermoelastic displacement potential
Michell’s function M as

and
(9)
(10)
(11)

and
(12)
where G and v are the shear modulus and Poisson’s ratio respectively.
For traction free surface stress functions
(13)
Equations (1) to (13) constitute mathematical formulation of the problem.

III.

SOLUTION

To obtain the expression for temperature T (r, z, t), we introduce the finite Hankel transform
over the variable r and its inverse transform defined by [6] as
(14)
(15)
where

,

(16)

are roots of transcendental equation
(17)
where

is Bessel function of the first kind of order n.

On applying the finite Hankel transform defined in the Eq. (14), its inverse transform defined in (15)
and applying Laplace transform and its inverse by residue method successively to the Eq. (2), one obtains the
expression for temperature as

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Quasi Static Thermal Stresses In A Limiting Thick…

(18)
where
,

Since initial temperature
(19)
Michell’s function M
Now let’s assume that Michell’s function M, which satisfy Eq.(7) is given by

(20)
where
and
are arbitrary functions, which can be determined by using condition (13).
Goodiers Thermoelastic Displacement Potential

Assuming the displacement function

which satisfies Eq. (1) as

(21)
Now using Eqs. (18), (20) and (21) in Eqs. (9), (10), (11) and (12), one obtains the expressions for stresses
respectively as

(22)

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Quasi Static Thermal Stresses In A Limiting Thick…

(23)

(24)

(25)
In order to satisfy condition Eq. (13), solving Eqs. (22) and (25) for

and

one obtains

(26)

(27)
where

IV.

SPECIAL CASE AND NUMERICAL CALCULATIONS

Setting
,
where
is well known diract delta function of argument r.
Material Properties

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59 | P a g e
Quasi Static Thermal Stresses In A Limiting Thick…
The numerical calculation has been carried out for steel (0.5% carbon) limiting thick circular plate with
the material properties defined as
Thermal diffusivity = 14.74
Specific heat
Thermal conductivity k = 53.6 W/m K,
Poisson ratio
Young’s modulus
Lame constant
,
Coefficient of linear thermal expansion
Roots of Transcendental Equation
The
of transcendental equation
help of mathematical software Mat lab.

are the roots
The numerical calculation and the graph has been carried out with the

V.

DISCUSSION

In this paper a limiting thick circular plate with internal heat generation is considered and determined
the expressions for temperature, displacement and stresses. We compute the effects of internal heat generation
and axisymmetric heat supply in terms of stresses along radial direction by substituting
in Eqs. (18), (21),
(22), (23), (24), (25), (26) and (27). We compare the results for
and
. As a special case
mathematical model is constructed by considering steel (0.5% carbon) limiting thick circular plate with the
material properties specified above.

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Quasi Static Thermal Stresses In A Limiting Thick…

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Quasi Static Thermal Stresses In A Limiting Thick…

From fig. 1 and 2, it is observed that due to internal heat generation in limiting thick circular plate
temperature increases along radial direction. Axisymmetric heat supply shows a negligible effect at the point of
heat supply along radial direction.
From fig. 3 and 4, it is observed that the internal heat generation and axisymmetric heat supply shows a
negligible effect on displacement in limiting thick circular plate at the point of heat supply along radial
direction.
From fig. 5 and 6, it is observed that the internal heat generation and axisymmetric heat supply
develops tensile radial stress
towards the lateral surface of limiting thick circular plate along radial direction.
From fig. 7 and 8, it is observed that the internal heat generation and axisymmetric heat supply develops tensile
angular stress towards the lateral surface of limiting thick circular plate along radial direction.
From fig. 9 and 10, it is observed that the internal heat generation and axisymmetric heat supply
develops tensile axial stress
towards the lateral surface of limiting thick circular plate along radial direction.
From fig. 11 and 12, it is observed that the internal heat generation and axisymmetric heat supply develops
infinitesimal stress
towards the lateral surface of limiting thick circular plate along radial direction.

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Quasi Static Thermal Stresses In A Limiting Thick…
VI.

CONCLUSION

We can conclude that due to internal heat generation in limiting thick circular plate temperature
increases along radial direction. Axisymmetric heat supply shows a negligible effect on temperature,
displacement at the point of heat supply in limiting thick circular plate along radial direction. The internal heat
generation and axisymmetric heat supply develops tensile radial stress
, angular stress , the axial stress
and the stress

towards the lateral surface of limiting thick circular plate along radial direction.

The results obtained here are useful in engineering problems particularly in the determination of state
of stress in a limiting thick circular plate and base of furnace of boiler of a thermal power plant and gas power
plant.

REFERENCES
[1]
[2]
[3]
[4]
[5]
[6]

V. S. Kulkarni and K. C. Deshmukh, Quasi static thermal stresses in a thick circular plate due to
axisymmetric heat supply, Int. J. of Appl. Math and Mech. 5(6), 2009, 38-50.
W. Nowacki, The state of stresses in a thick circular disk due to temperature field, Bull. Acad. Polon. Sci.,
Scr. Scl. Tech., 5, 1957, 227.
C. M. Bhongade and M. H. Durge, An inverse steady state thermal stresses in a thin clamped circular plate with internal heat generation,
American Journal of Engineering Research,2(10), 2013, 276-281.
C. M. Bhongade and M. H. Durge, Effect of Michell function on steady state behavior of thick circular plate, IOSR Journal of
Mathematics,8(2), 2013, 55-60.
Naotake Noda, Richard B Hetnarski and Yoshinobu Tanigawa, Thermal Stresses, 2 nd edn., (Taylor and
Francis New York, 2003), 259-261.
M. N. Ozisik, Boundary Value Problems of Heat Conduction, International Text Book Company,
Scranton, Pennsylvania, 1968.

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63 | P a g e

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International Journal of Mathematics and Statistics Invention (IJMSI)

  • 1. International Journal of Mathematics and Statistics Invention (IJMSI) E-ISSN: 2321 – 4767 P-ISSN: 2321 - 4759 www.ijmsi.org Volume 1 Issue 2 ǁ December. 2013ǁ PP-56-63 Quasi Static Thermal Stresses in A Limiting Thick Circular Plate with Internal Heat Generation Due To Axisymmetric Heat Supply C. M. Bhongade1 and M. H. Durge2 1 2 Department of Mathematics, Shri. Shivaji College,Rajura, Maharashtra, India Department of Mathematics, Anand Niketan College, Warora, Maharashtra, India ABSTRACT: The present paper deals with the determination of quasi static thermal stresses in a limiting thick circular plate with internal heat generation subjected to axisymmetric arbitrary heat flux on upper and lower surface and the fixed circular edge is thermally insulated. Initially the plate is at zero temperature. Here we modify Kulkarni [1]and compute the effects of internal heat generation and axisymmetric heat supply in terms of stresses along radial direction. The governing heat conduction equation has been solved by the method of integral transform technique. The results are obtained in a series form in terms of Bessel’s functions. The results for temperature change, displacement and stresses have been computed numerically and illustrated graphically. KEYWORDS: Quasi static thermal stresses, limiting thick circular plate, internal heat generation, axisymmetric heat supply. I. INTRODUCTION During the last century the theory of elasticity has found of considerable applications in the solution of engineering problems. Thermoelasticity contains the generalized theory of heat conductions, thermal stresses. A considerable progress in the field of air-craft and machine structures, mainly with gas and steam turbines and the emergence of new topics in chemical engineering have given rise to numerous problems in which thermal stresses play an important role and frequently even a primary role. Nowacki [2] has determined the temperature distribution on the upper face, with zero temperature on the lower face and the circular edge thermally insulated. Bhongade and Durge [3] studied an inverse steady state thermal stresses in a limiting thick circular plate with internal heat generation. Most recently Bhongade and Durge [4] considered thick circular plate and discuss the effect of Michell function on steady state behavior of thick circular plate, now here we consider a thick circular plate with internal heat generation subjected to axisymmetric arbitrary heat flux on upper and lower surface and the fixed circular edge is thermally insulated. Initially the plate is at zero temperature. Here we modify Kulkarni [1] and compute the effects of internal heat generation and axisymmetric heat supply on the limiting thick circular plate in terms of stresses along radial direction. The governing heat conduction equation has been solved by the method of integral transform technique. The results are obtained in a series form in terms of Bessel’s functions. The results for temperature change, displacement and stresses have been computed numerically and illustrated graphically. A mathematical model has been constructed with the help of numerical illustration by considering steel (0.5% carbon) limiting thick circular plate. No one previously studied such type of problem. This is new contribution to the field. The direct problem is very important in view of its relevance to various industrial mechanics subjected to heating such as the main shaft of lathe, turbines and the role of rolling mill, base of furnace of boiler of a thermal power plant and gas power plant. II. FORMULATION OF THE PROBLEM Consider a limiting thick circular plate of radius a and thickness 2h defined by Initially the plate is at zero temperature. Let the plate be subjected to a axisymmetric arbitrary heat flux prescribed over the upper surface and the lower surface The fixed circular edge is thermally insulated. Assume a limiting thick circular plate with internal heat generation is free from traction. Under these prescribed conditions, the quasi static transient thermal stresses are required to be determined. The differential equation governing the displacement potential function is given in [5] as www.ijmsi.org 56 | P a g e
  • 2. Quasi Static Thermal Stresses In A Limiting Thick… (1) where K is the restraint coefficient and temperature change is initial temperature. Displacement function is known as Goodier’s thermoelastic displacement potential. The temperature of the plate at time t satisfying the heat conduction equation as follows, (2) with the boundary conditions (3) (4) (5) and the initial condition at (6) where is the thermal diffusivity of the material of the plate, k is the thermal conductivity of the material of the plate, q is the internal heat generation and is well known dirac delta function of argument r. The Michell’s function M must satisfy (7) where (8) The components of the stresses are represented by the thermoelastic displacement potential Michell’s function M as and (9) (10) (11) and (12) where G and v are the shear modulus and Poisson’s ratio respectively. For traction free surface stress functions (13) Equations (1) to (13) constitute mathematical formulation of the problem. III. SOLUTION To obtain the expression for temperature T (r, z, t), we introduce the finite Hankel transform over the variable r and its inverse transform defined by [6] as (14) (15) where , (16) are roots of transcendental equation (17) where is Bessel function of the first kind of order n. On applying the finite Hankel transform defined in the Eq. (14), its inverse transform defined in (15) and applying Laplace transform and its inverse by residue method successively to the Eq. (2), one obtains the expression for temperature as www.ijmsi.org 57 | P a g e
  • 3. Quasi Static Thermal Stresses In A Limiting Thick… (18) where , Since initial temperature (19) Michell’s function M Now let’s assume that Michell’s function M, which satisfy Eq.(7) is given by (20) where and are arbitrary functions, which can be determined by using condition (13). Goodiers Thermoelastic Displacement Potential Assuming the displacement function which satisfies Eq. (1) as (21) Now using Eqs. (18), (20) and (21) in Eqs. (9), (10), (11) and (12), one obtains the expressions for stresses respectively as (22) www.ijmsi.org 58 | P a g e
  • 4. Quasi Static Thermal Stresses In A Limiting Thick… (23) (24) (25) In order to satisfy condition Eq. (13), solving Eqs. (22) and (25) for and one obtains (26) (27) where IV. SPECIAL CASE AND NUMERICAL CALCULATIONS Setting , where is well known diract delta function of argument r. Material Properties www.ijmsi.org 59 | P a g e
  • 5. Quasi Static Thermal Stresses In A Limiting Thick… The numerical calculation has been carried out for steel (0.5% carbon) limiting thick circular plate with the material properties defined as Thermal diffusivity = 14.74 Specific heat Thermal conductivity k = 53.6 W/m K, Poisson ratio Young’s modulus Lame constant , Coefficient of linear thermal expansion Roots of Transcendental Equation The of transcendental equation help of mathematical software Mat lab. are the roots The numerical calculation and the graph has been carried out with the V. DISCUSSION In this paper a limiting thick circular plate with internal heat generation is considered and determined the expressions for temperature, displacement and stresses. We compute the effects of internal heat generation and axisymmetric heat supply in terms of stresses along radial direction by substituting in Eqs. (18), (21), (22), (23), (24), (25), (26) and (27). We compare the results for and . As a special case mathematical model is constructed by considering steel (0.5% carbon) limiting thick circular plate with the material properties specified above. www.ijmsi.org 60 | P a g e
  • 6. Quasi Static Thermal Stresses In A Limiting Thick… www.ijmsi.org 61 | P a g e
  • 7. Quasi Static Thermal Stresses In A Limiting Thick… From fig. 1 and 2, it is observed that due to internal heat generation in limiting thick circular plate temperature increases along radial direction. Axisymmetric heat supply shows a negligible effect at the point of heat supply along radial direction. From fig. 3 and 4, it is observed that the internal heat generation and axisymmetric heat supply shows a negligible effect on displacement in limiting thick circular plate at the point of heat supply along radial direction. From fig. 5 and 6, it is observed that the internal heat generation and axisymmetric heat supply develops tensile radial stress towards the lateral surface of limiting thick circular plate along radial direction. From fig. 7 and 8, it is observed that the internal heat generation and axisymmetric heat supply develops tensile angular stress towards the lateral surface of limiting thick circular plate along radial direction. From fig. 9 and 10, it is observed that the internal heat generation and axisymmetric heat supply develops tensile axial stress towards the lateral surface of limiting thick circular plate along radial direction. From fig. 11 and 12, it is observed that the internal heat generation and axisymmetric heat supply develops infinitesimal stress towards the lateral surface of limiting thick circular plate along radial direction. www.ijmsi.org 62 | P a g e
  • 8. Quasi Static Thermal Stresses In A Limiting Thick… VI. CONCLUSION We can conclude that due to internal heat generation in limiting thick circular plate temperature increases along radial direction. Axisymmetric heat supply shows a negligible effect on temperature, displacement at the point of heat supply in limiting thick circular plate along radial direction. The internal heat generation and axisymmetric heat supply develops tensile radial stress , angular stress , the axial stress and the stress towards the lateral surface of limiting thick circular plate along radial direction. The results obtained here are useful in engineering problems particularly in the determination of state of stress in a limiting thick circular plate and base of furnace of boiler of a thermal power plant and gas power plant. REFERENCES [1] [2] [3] [4] [5] [6] V. S. Kulkarni and K. C. Deshmukh, Quasi static thermal stresses in a thick circular plate due to axisymmetric heat supply, Int. J. of Appl. Math and Mech. 5(6), 2009, 38-50. W. Nowacki, The state of stresses in a thick circular disk due to temperature field, Bull. Acad. Polon. Sci., Scr. Scl. Tech., 5, 1957, 227. C. M. Bhongade and M. H. Durge, An inverse steady state thermal stresses in a thin clamped circular plate with internal heat generation, American Journal of Engineering Research,2(10), 2013, 276-281. C. M. Bhongade and M. H. Durge, Effect of Michell function on steady state behavior of thick circular plate, IOSR Journal of Mathematics,8(2), 2013, 55-60. Naotake Noda, Richard B Hetnarski and Yoshinobu Tanigawa, Thermal Stresses, 2 nd edn., (Taylor and Francis New York, 2003), 259-261. M. N. Ozisik, Boundary Value Problems of Heat Conduction, International Text Book Company, Scranton, Pennsylvania, 1968. www.ijmsi.org 63 | P a g e