Problem Specification
High density polyethylene pipe (20 mm diameter) is rolled into sixteen coils. Groups of eight coils are mounted on two sleds. Each coil has a radius of 1 m and a length of approximately 75 m. The coil groups are connected to feed and return piping with a diameter of 50 mm (see Figure 10). The coil groups are 2.4 m in height and sit at the bottom of a pond that is 6 m deep. The total length of the piping is 1446 m.
Figure 10: Polyethylene pipe system. Elevation above the pond bottom is indicated. Feed and return piping (gray) is 50 mm in diameter while coils (black) are 20 mm in diameter. The pipes are insulated above the pond surface.
The heat exchange between pond water and pipe fluid will depend, among other things, on the temperature difference between the two. A slow current in the pond will make the heat transfer more effective than water at rest. The pond is warmer closer to the surface, as shown by the temperature data in the table below.
It is easy to set up a function in the software with linear interpolation between points so that the varying pond temperature can be taken into account in the simulation.
Flow Equations
The stationary momentum and continuity equations below describe the stationary flow inside the pipe system, and are solved by the Nonisothermal Pipe Flow interface:
(1)
(2)
Above, A (SI unit: m2) is the cross section area of the pipe, ρ (SI unit: kg/m3) is the density, u (SI unit: m/s) is the fluid velocity in the tangential direction of the pipe curve segment, and p (SI unit: N/m2) is the pressure. F (SI unit: N/m3) is a volume force, like gravity.
Gravity can be included explicitly in the model, but since the variation in density is negligible, and the model is not pressure driven, the only effect of including gravity is a change in the total pressure level. It is therefore common modeling practice to exclude gravity from F and interpret the pressure variable as the reduced pressure , where z0 is the datum level of the free liquid surface. This reduces the model complexity and yields the same results. For models where you want to include gravity effects you can add a Volume Force node.
Expressions for the Darcy Friction Factor
The last two terms of Equation 1 describes the pressure drop due to internal viscous shear and gravity. One of the terms contain the Darcy friction factor, fD, which is a function of the Reynolds number and the surface roughness divided by the hydraulic pipe diameter, e/dh. The Nonisothermal Pipe Flow interface provides a library of built-in expressions for the Darcy friction factor, fD.
Figure 11: Select a shape and different predefined friction models in the Pipe Properties node.
This example uses the Churchill relation (Ref. 1) that is valid for laminar flow, turbulent flow, and the transitional region in between. The Churchill relation is:
(3)
where
(4)
(5)
As seen from the equations above, the friction factor is a function of the surface roughness divided by diameter of the pipe. Surface roughness data can be selected from a predefined list in the Pipe Properties feature.
Figure 12: Specify the surface roughness in the Pipe Properties node.
The Churchill equation is also a function of the fluid properties, through the Reynolds number:
(6)
The physical properties of water as a function of temperature are directly available from the software’s built-in material library. Inspection of Equation 3 reveals that for low Reynolds numbers (at laminar flow), the friction factor is 64/Re, and for very high Reynolds numbers, the friction factor is independent of Re.
Heat Transfer Equations
The energy equation for the pipeline flow is:
(7)
where Cp (SI unit: J/(kg·K)) is the heat capacity at constant pressure, T is the temperature (SI unit: K), and k (SI unit: W/(m·K)) is the thermal conductivity. The second term on the right-hand side of Equation 7 corresponds to friction heat dissipated due to viscous shear. Qwall (SI unit: W/m) is a source/sink term due to heat exchange with the surroundings through the pipe wall:
(8)
where Z (m) is the wetted perimeter of the pipe, h (W/(m2·K)) is an overall heat transfer coefficient and Text (K) is the external temperature outside of the pipe.
If there are several wall layers, the overall heat transfer coefficient includes contributions from internal film resistance, layered wall resistance, and external film resistance. The heat transfer coefficient is automatically calculated taking all of these resistances into account.
In this model we only have one wall and the properties of the pipe wall are given in the table below.
dwall
kwall