Heller Dry Cooling Tower CFD Simulation

Price: $20

In this project, the airflow inside a dry cooling tower (HELLER) is simulated and analyzed by ANSYS Fluent.

Audio: English
Subtitles: English, Spanish, Arabic, Turkish, French, Portuguese
Intermediate
1 Lesson
14m 43s
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  • Electrical & Power

    Heller Dry Cooling Tower CFD Simulation

    Price: $20

    In this project, the airflow inside a dry cooling tower (HELLER) is simulated and analyzed by ANSYS Fluent.

    Audio: English
    Subtitles: English, Spanish, Arabic, Turkish, French, Portuguese
    Intermediate
    1 Lesson
    14m 43s

    Heller Dry Cooling Tower CFD Simulation, ANSYS Fluent Training

    A dry cooling tower is used as a means of indirect heat transfer between the working fluid (water) and the coolant(air). In a thermal plant, the working fluid (water) exits the condensers and then is pumped into a ring of heat exchangers. These heat exchangers are air-cooled, which means that they are cooled by natural air suction caused by a temperature difference between the inside and the outside of the cooling tower.

    The more the temperature difference exists between outside air and working fluid, the stronger the temperature driving force. In the summer, the temperature difference between the working fluid and the ambient air decreases, which will result in a reduction in temperature driving force, making the cooling tower’s efficiency to decrease.

    Therefore, the thermal unit has to lower its power production, and the rate of water consumption will increase drastically to cool the heat exchangers. In this project, the airflow inside a dry cooling tower (HELLER) is simulated and analyzed by ANSYS Fluent.

    Heller Geometry & Mesh

    The geometry of this project includes a cooling tower, heat exchanger, flow domain, and an air inlet. The geometry is designed and meshed inside GAMBIT. The mesh type used for this geometry is unstructured and the total element number is 1343988 cells.

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    CFD simulation

    The assumptions considered in this project are:

    • Simulation is done using a pressure-based solver.
    • The present simulation and its results are considered to be steady and do not change as a function time.
    • The effect of gravity has been taken into account and is equal to -9.81m/s2 in the Y direction.

    The applied settings are recapitulated in the following table.

    (Heller)Models
    Viscous modelk-epsilon
    k-epsilon modelstandard
    near-wall treatmentstandard wall function
    Energyon
    (Heller)Boundary conditions
    InletPressure inlet
    Gauge total pressure0 Pa
    Direction specification methodNormal to boundary
    OutletPressure outlet
    Gauge pressure0 Pa
    Backflow direction specification methodNormal to boundary
    temperature303 K
    Walls
    Heller, Heller shadowwall motionstationary wall
    Wall, wall shadowheat flux0 W/m-2
    wall motionstationary wall
    RadiatorTemperature318 K
    Heat generation rate14861.52 W/m3
    wall motionstationary wall
    Radiator shadowTemperature313 K
    Heat generation rate14861.52 W/m3
    (Heller)Solution Methods
    Pressure-velocity coupling SIMPLE
    Spatial discretizationpressurestandard
    densityfirst-order upwind
    momentumfirst-order upwind
    energyfirst-order upwind
    turbulent kinetic energyfirst-order upwind
    turbulent dissipation ratefirst-order upwind
    (Heller)Initialization
    Initialization method Standard
    gauge pressure0 Pa
    velocity (x,y,z)0 m/s-1
    temperature303.0806 K
    Turbulent kinetic energy1 m2/s2
    Turbulent dissipation rate1 m2/s3

    Heller Results

    The contours of velocity, pressure, temperature, and flow streamlines are obtained at the end of the solution process.