^{1}

^{*}

^{2}

^{3}

^{4}

In this paper, analysis of post-treatment of wire coating is presented. Coating material satisfies power law fluid model. Exact solutions for the velocity field, volume flow rate and average velocity are obtained. Moreover, the heat transfer results are presented for different cases of linearly varying on the boundaries. The variations of velocity, volume flow rate, radius of coated wire, shear rate and the force on the total wire are presented graphically and discussed.

The wire coating process is basically an extrusion operation in which either the molten polymer, in the form of tubing, is extruded continuously over axially moving wire, or the wire is pulled through the extruded molten polymer. Polymer extrudate is an important industrial process used for coating a wire for primary insulation of conducting wires with molten polymers for mechanical strength and environmental protection purposes. Wire coating have many application in the field of chemical and industrial engineering. Many authors have studied the wire coating phenomena.

The basic concept of modeling the wire coating for viscous fluid is given in the books by Denn and middleman [1,2]. McKelvey [

The coated wire after leaving the die is effected by the quality of the material used in coating process, the wire drawing velocity and the temperature. There are very few disclosures presenting theoretical analysis of flow in the posttreatment process subsequent to the die.

The analysis of the drag flow of the coated polymer outside pressure die was carried out by Kasajima and Katsuhiko Ito [

• Temperature of the wire is constant while it is varying linearly on the surface of the coated wire.

• Temperature of the wire varying linearly while it is constant on the surface of the coated wire.

• Temperature of the wire and the surface of coated wire are varying linearly at the same temperature gradient.

The non-linear differential equations governing the model are made dimensionless and solved for velocity and temperature distribution. Theoretical analysis on the drag flow mechanism of polymer extrudate, in the heat treatment process, is presented.

The basic equations governing the flow of an incompressible fluid with thermal effects are:

where is the velocity vector, is the constant density, is the body force, is the Cauchy stress tensor, denote the material derivative, is the fluid temperature, is the thermal conductivity, is the specific heat and is the gradient of velocity vector.

The Cauchy stress tensor is defined as

In which is the pressure, is the identity tensor and is the extra stress tensor. For power law fluid model is defined as

, (5)

where

where is the scalar invariant, is the coefficient of viscosity of the fluid, in superscript denotes the transpose of the matrix, is the consistency index and is the power law index. The index is non-dimensional and the dimension of depends on the value of. The parameter subdivide fluids into pseudoplastic fluids, dilatant fluids and Newtonian fluid For. Therefore the deviation of from unity indicates the degree of deviation from Newtonian behavior [

In wire coating process, the quality of the polymer and wire drawing velocity are important within the die, after leaving the die temperature and the shape of the transverse sectioning is also very important. Consider the flow of the polymer extrudate given in

Consider the wire of radius is dragged in the direction with velocity through an incompressible polymer satisfying power law fluid model (II) and the gas (III) surrounding the polymer (II) is flowing with a velocity in the direction.

Consider the cylindrical coordinates such that is perpendicular to the direction of flow.

Assume that:

1) The flow is incompressible due to the high viscosity of the polymer.

2) Polymer II holds the power law fluid model for shear rate.

3) In

Also assume that the flow is steady, laminar, unidirectional and axisymmetric:

We seek the velocity field of the form

then the boundary conditions for the problem become

In the flow through the tube, the scalar invariant is:

Substituting Equation (9) into Equation (6) one obtains:

Using the velocity field (7) the continuity Equation (1) is satisfied identically, and the non zero components of Equation (5) with the help of Equation (10) become:

Substituting the velocity field and Equation (11) in the momentum Equation (2) neglecting the body force take the form:

If the z-axis is chosen correspond to the direction of increasing pressure, polymer (II) moves in the minus direction of the z-axis and the shear ratebecomes plus for all value of Therefore, the absolute value of Equation (5) can be discarded.

Equation (14) represents the flow due to pressure gradient. After leaving the die, there is only drag flow. Hence, we consider

and the energy Equation (3) becomes:

For linearly varying temperature, consider

where is the temperature gradient.

Substituting Equation (17) into Equation (16), we have

Now first the velocity field is determined from Equation (15) and then the temperature distribution can be easily calculated using Equation (18).

The average velocity is

At some control surface downstream, the volume flow rate of coating is

where is the radius of the coated wire.

The volume flow rate of the polymer is

The thickness of the coated wire can be obtained from Equations (16) and (17) as

The force on the wire is computed by determining the shear stress at the wire surface. This is given by

The force on the total wire surface is

Introduce the dimensionless parameters

Equations (8), (15) and (18)-(25) after dropping the “” take the following form:

The solution to (26) corresponding to the boundary conditions (27) are:

For, the velocity field can be obtain from Equation (26).

where the superscript “” means the case of.

For the average velocity is obtained from Equations (29) and (34):

For the average velocity is obtained from Equations (29) and (35):

For the shear rate can be obtained from Equation (34):

For the shear rate is obtained from Equation (35) as:

The thickness of the coated wire for is obtained from Equations (31) and (34):

Similarly, the thickness of the coated wire for is obtained from Equations (31) and (35):

In a similar manner, the force on the total wire surface for power law index is not equal to 1 is

and the force on the total wire surface for the case when the power law index is equal to 1 is given by

In dimensionless form the volume flow rate for is or is not equal to 1are the same as the average velocity in Equations (37) and (36) respectively.

In case of transformation of our problem to original parameters the results of velocity field, volume flow rate, average velocity and rate of shear stress are transformed to the results of Kasajima and Katsuhiko Ito [

Keeping the importance of temperature in our problem we are seeking the temperature distribution with different cases.

Case 1. Temperature of the wire is constant while it is varying linearly on the surface of the coated wire:

Here, consider the temperature of the wire is, and it is on the surface of the coated wire, so from Equation (17) we have

After transformation we obtain

where

.

For the velocity field from Equation (23) is substitute in Equation (22) and solved corresponding to the boundary conditions (45), we obtain the expression for temperature distribution in form of as:

For the velocity field from Equation (24) is substitute in Equation (22) and solved corresponding to the boundary conditions (45), the explicit function for is obtained for temperature field as:

Case 2. Temperature of the wire varying linearly while it is constant on the surface of the coated wire:

In this case, consider the temperature at the surface of wire is, and on the surface of continuum.

Under the above consideration Equation (17) gives

After transformation of the boundary conditions (48) for the non-dimensional temperature distribution takes the following form

where

.

For the velocity field from Equation (22) is substitute in Equation (22) and solved corresponding to the boundary conditions (49), we have

For the velocity field from Equation (24) is substitute in Equation (22) and solved corresponding to the boundary conditions (49), we have

Case 3. Temperature of the wire and the surface of coated wire are varying linearly at the same temperature gradient:

Consider the temperatures at the surface of wire and on the surface of continuum are.

From Equation (17), we have

After simplification according to demand of our problem, we obtain

For the velocity field from Equation (22) is substitute in Equation (22) and solved corresponding to the boundary conditions (53), we have

For the velocity field from Equation (24) is substitute in Equation (22) and solved corresponding to the boundary conditions (53), after simplification we have

The posttreatment of wire coating analysis are carried out for power law model fluid. The velocity field, volume flow rate, average velocity, force on the total wire, thickness of coated wire and shear rate have been derived for is or is not equal to 1. In posttreatment problem the temperature is extremely important for cooling the wire. Therefore, regarding the importance of temperature we have discussed three cases for linearly varying temperature. Expression for temperature distributions in non-dimensional form are obtained for and. The interpretations of the results are carried out under the influence of non-dimensional parameters. It is concluded that the velocity decreases as the power law index increases. In addition, the non-Newtonian parameter decrease the fluid velocity. Also, it is concluded that the force on the coated wire increases as the velocity ratio increases and decreases while increases. It is observed that for the thickness of coated wire increases. Moreover, with a linearly varying wall temperature along the direction of flow the highest temperature rise in the centre of the channel depends on the dimensionless number. One can see the behavior of the physical quantities such as velocity function, non-dimensional function of temperature profile and the differential form of these functions from Figures 3-15.

The first author is thankful to higher education commission of Pakistan for funding in MS leading to PhD studies under the 5000 indigenous scholarship scheme BatchIV.