# Internal Flow of a pipe CFD Simulation in Different Flow Regimes

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The purpose of the present simulation is to study and compare fluid flow in different flow regimes in a pipe.

This product includes a Mesh file and a comprehensive Training Movie.

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## Description

## Project Description of Internal Flow with Different Flow Regimes

The present problem simulates the internal flow of water through a simple horizontal pipe, which due to the symmetrical structure of this pipe, half of its geometry consists of a semi-cylinder has been studied. The purpose of the present simulation is to study and compare fluid flow in different flow regimes. For this purpose, this simulation is performed in three modes, which include laminar flow, k-Ԑ turbulence flow and k-ω turbulence flow. Laminar flow indicates the regular and uniform movement of fluid layers on top of each other and the absence of flow turbulence, including vortices.

Turbulent flow, on the other hand, indicates irregular motion of fluid particles with very large irregular vortices. To determine the type of flow regime, one must pay attention to the Reynolds number defined for the flow and compare its value with the critical Reynolds value in the mentioned geometric model. If the Reynolds number is greater than the critical Reynolds value, the flow is turbulent, and if the Reynolds number is less than the critical Reynolds value, it is laminar flow.

## Project Description

Therefore, since the Reynolds number depends on the amount of flow inlet velocity, in the current simulation, the value of the inlet velocity is considered variable; So that for the first case, which is the laminar flow, the inlet flow velocity is considered to be 0.0176 m.s-1, and in the second and third cases, which are turbulent flow, the inlet flow velocity is considered to be 0.334 m.s-1. In general, laminar flow consists of solving one equation and turbulence flow consists of solving two equations.

The k-epsilon RNG turbulence model is used to model transient flows, flows in geometries with high curvatures, and air conditioning problems; While the k-omega standard turbulence model for modeling currents including velocity deceleration and separation due to reverse pressure gradient, mixing layer flows and plate and radial jets, high rotational flows, and issues related to aerodynamic forces and turbochargers are applicable.

## Geometry & Mesh

The 3-D geometry of the model is designed using design modeler software. The present model consists of a semi-cylinder with a radius of 0.015 m and a length of 1 m. The following figure shows a view of the graphic geometry.

The meshing of the model has been done using ANSYS Meshing software and the mesh type is structured. The element number is 23120. The following figure shows the mesh.

## CFD Simulation Setting of Internal Flow Considering Different Flow Regimes

To simulate the present model, several assumptions are considered:

- We perform a pressure-based solver.
- The simulation is steady.
- The gravity effect on the fluid is ignored.

A summary of the defining steps of the problem and its solution is given in the following table:

Models |
||

variable | Viscous model | |

Boundary conditions |
||

velocity inlet | Inlet | |

0.0167 m.s^{-1} for laminar |
velocity magnitude | |

0.334 m.s^{-1} for turbulence |
||

pressure outlet | Outlet | |

0 Pascal | gauge pressure | |

Wall | Wall | |

stationary wall | wall motion | |

Solution Methods |
||

SIMPLE | |
Pressure-velocity coupling |

Second order | pressure | Spatial discretization |

Second order upwind | momentum | |

Initialization (internal flow) |
||

Standard | Initialization method | |

0 Pa | gauge pressure | |

0 m.s^{-1} |
x-velocity , y-velocity | |

0.0167 m.s^{-1} for laminar |
z-velocity | |

0.334 m.s^{-1} for turbulence |

** Different Flow Regime **Results

At the end of the solution process, we obtain two-dimensional and three-dimensional turbulence pressure, velocity and kinetic energy contours in three modes: laminar flow, k-epsilon RNG turbulence flow and k-omega standard turbulence flow. We display two-dimensional contours on the center plate of the pipe, which is a symmetrical plate. Also, we present velocity and pressure diagrams in terms of location in the central axis of the pipe for two different modes of turbulence flow.

There are a Mesh file and a comprehensive Training Movie that presents how to solve the problem and extract all desired results.

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