As.Prof. Amirtayev Kanat

A.Yasawi International Kazakh-Turkish University, Kazakhstan

 

NUMERICAL ALGORITHMS TO ANALIZ THE STATE OF

TOTAL THERMAL ENERGY OF AN ELASTIC ROD

 


 

Today, the existing studies of thermo-elastic state of one-dimensional elements of the construction are relatively of private character and are not subject to all exploitation conditions [1-4]. Also, very important tasks of technology and chemical engineering, thermo elastic steady state of one-dimensional construction elements with axial force, unequal distribution of temperature field, thermal flow, heat exchange and thermal insulation are worth careful studying.

Earlier the authors made the fundamental justification for the fact that the function which gives the minimum to the functional that characterizes the full thermal energy is the solution to of the heat-transfer equation with the appropriate natural boundary conditions [2]. The field of temperature distribution along the rod length, with rod lengthening and tensile strength was defined.

The differential equation for temperature distribution along the full rod length of the rod was considered:

      (1)

 

With the following boundary conditions:

             (2)

 

If the coefficient of thermal expansion of the rod material is , then the lengthening of the rod due to field of temperature distribution is

        (3)

To compare our results with those obtained by other authors, the parameter values representing the geometric, physical and mechanical and thermal properties of the rod are defined as follows:

 

;; ; ; ;; ;

 

The temperature values in the points, , of the rod will be:

 

These found values exactly coincide with the values found previously. Extension of the rod due to the impact of the tensile strength has the following form

       (4)

Then, using (3), (4) the value of the ratio is

          (5)

If,

Then for the rod under consideration there will be .

As it can be seen, here it is necessary to take into account the fact that the extension of the rod due to the temperature will be much more considerable than the extension of the rod due to the applied tensile force, when the rod structural elements are under the influence of heat flow and tensile strength.

Here the numerical study of lengthening of partially heat-isolated rod in the presence of a heat sources and tensile strength is given. The numerical study with the different source data was conducted.

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Fig. 1. Calculation scheme of the task

 

To do it, the rod with length L will be to discrete quadratic finite elements with three nodes.

Then, for the final elements in the heat isolated lateral surface parts, the view of the functional, expressing conservation and change of the total thermal energy is as follows

(6)

For the finite element heat isolated by the lateral surface, the functional type is as follows

(7)

On the lateral surface of the rod, the heat exchange with the environment takes place.

(8)

On the lateral surface of the rod, the heat exchange with the environment takes place as well.(9)

Then, for the rod in general, the expression of the corresponding functional is as follows

(10)

The influence of temperature and tensile strength on the lengthening of the rod was analyzed [1].

Moreover, the lengthening of considered rod is affected the by heat transfer coefficientbetween the rod material and the cross-sectional area of the clamped rod ends [2].

After testing of the developed computational algorithm, the influence of local temperature and heat exchange on the thermal-strained and deformed state of the test rod is analyzed. To do this, the values ​​of the compressive force and the true stress on different rod parts are calculated [1].The influence of the heat flow on the thermal strained deformed and state of the test rod was analyzed [2].

The analysis of the effect of heat flow on the cross-sectional area and analyses of the effect of the heat exchange with the environment through a portion of the lateral surface on the thermal-strained and deformed state of the test rod were carried out. These results are shown in Fig. 2-3.


 

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Fig. 2.The field of temperature distribution       Fig. 3.The law on the distribution

      along the length of the rod                                of displacements of nodal points along the rod length.

 

On the basis of the minimization of the functional characterizing the full thermal energy using quadratic finite elements with three nodes, the computational algorithm of tasks of determining the temperature distribution field in the rods of limited length in the presence of heat flow, heat exchange and partial insulation was constructed.

The corresponding developed computational algorithms were tested by several test problems.

The corresponding calculation algorithm of numerical study of thermal strained and deformed state of the rod partially thermally insulated and clamped by two ends, in the presence of the local temperature and heat exchange, was developed.

 

references

 

1.                       Kudaykulov A.K., Amirtayev K.B., Tuleuova R., Utebaev U.B., Tokkuliev B.M. Steady thermal stress-strained and deformed state of the rod in the presence of heat sources // Proceedings of the Fifth All-Russian scientific conference with international participation "Mathematical modeling and boundary value problems" - Samara - 2008. - p. 161-165.

2.                       Kudaykulov A.K., Amirtayev K.B., Utebaev U.B. Numerical study of strain-deformed state of the rod filled-rigidly at both ends, when exposed along the length to the parabolic law of the temperature field// Materialy IV mezinarodni vedecko-prakticka conference «Íàó÷íî ïðîñòðàíñòâî íà åâðîïà-2008». – Sofia – 2008. – Ò.28, – p. 21–24.

3.  AmirtayevK.B., UtebaevU.B., TokkulievB.M., ZhumadillaevaA. Determination of the law of temperature distribution in a partially insulated tube of limited length, with the heat flow on the inner bounded surface of closed mid-pipe // Materialy IV mezinarodni vedecko-prakticka conference «Áúäåùåòî ïðîáëåìèòå íà ñâåòîâíàòà íàóêà-2008». – Sofia – 2008. – p. 66–69.