Fluid Film Boiling Models Reference

The multi-component liquid film boiling models model vaporization above boiling temperature. These models assumes that boiling takes place either on hot film walls or inside film cells. Boiling at hot walls increases the heat flux between the film and the wall.

In a fluid film simulation, the Habchi Boiling model and the Rohsenow Boiling model are used to model the heat transfer rates from the film and predict the wall heat flux due to boiling.

Theory See Boiling.
Model Names Habchi Boiling

Rohsenow Boiling

Provided By [phase interaction] > Models > Boiling Model
Example Node Path Continua > Physics 1 > Models > Multiphase Interaction > Phase Interactions > [phase interaction] > Models > Habchi Boiling
Continua > Physics 1 > Models > Multiphase Interaction > Phase Interactions > [phase interaction] > Models > Rohsenow Boiling
Requires Physics continuum selections:
  • Single phase physics continuum with Multi-Component Gas.
  • Optional Models: Coupled Energy, Segregated Fluid Enthalpy or Segregated Fluid Temperature
  • The Fluid Film model activated, with the fluid film phase defined as a Multi-Component Liquid.
  • Fluid Film Coupled Energy: Coupled Temperature or
  • Fluid Film Segregated Energy: Segregated Fluid Film Temperature

A Film-Physics Continuum Interaction phase interaction is required.

Phase interaction selections:
  • Optional Models: Component Mapping
Properties Key properties are:

Habchi Boiling: See Habchi Boiling Model Properties.

Rohsenow Boiling: See Rohsenow Boiling Model Properties.

Activates Model Controls (child nodes) Rohsenow Boiling: HTCxArea

Habchi Boiling: Minimum Length, Thermal Boundary Height

Materials Heat of Formation, Latent Heat of Vaporization, Saturation Pressure, Standard State Temperature, Critical Temperature, Critical Pressure, Leidenfrost Temperature, Nukiyama Temperature.

See Material Properties.

Field Functions See Field Functions.

Rohsenow Boiling Model Properties

Boiling Model Parameter c_sf
Characterizes the fluid wall interface. c s f in Eqn. (2802).
n
The Prandtl Number Exponent. n in Eqn. (2802).
Boiling Model Parameter c_s
Parameter that is used to compute the wall heat flux. c s in Eqn. (2806).
Constant of Critical Heat Flux
c m a x in Eqn. (2803).
Constant of Minimal Heat Flux
c m i n in Eqn. (2804).
Wall Boiling Evaporation Factor c_e
The wall boiling evaporation c e factor that determines how much of the boiling heat flux generates vapor. See Eqn. (2807).

Habchi Boiling Model Properties

Dry Area Fraction
The dry area fraction coefficient which sets the strength of the boiling rate through the vapor cushion. This value is β 2 in Eqn. (2818).
Under-Relaxation Factor
The heat flux under-relaxation factor.

HTCxArea

The HTCxArea node applies to Rohsenow Boiling.

The HTCxArea node represents the heat transfer coefficient ( W / m 2 K ) between the vapor bubbles and the surrounding liquid, which is multiplied by the specific contact area (contact area per unit volume, m 2 / m 3 ) between the two.

Minimum Length

Available when using the Habchi Boiling model.

Sets the method for calculating the minimum contact lines length density k c l l d min in Eqn. (2822).
Method Corresponding Method Properties
Habchi

Computes the minimum length k c l l d min with the Habchi method according to Eqn. (2823).

Surface Roughness
Specifies R u in Eqn. (2823)
Roughness Prefactor
Specifies k R u 1 in Eqn. (2823)
Roughness Power Exponent
Specifies k R u 2 in Eqn. (2823)
Constant, Field Function Specifies k c l l d min as a scalar value.
User Code
Function
Specifies k c l l d min as a user-defined function.

Thermal Boundary Height

Available when using the Habchi Boiling model.

Sets the method for calculating the thermal boundary height δ t h in Eqn. (2812) .
Method Corresponding Method Properties
Evaporation

Computes the thermal boundary height with the evaporation method. This method estimates the value of δ t h based on the maximum evaporation rate.

Maximum Evaporation Rate
Specifies the maximum evaporation rate, m C H F . at critical heat flux, or Nukiyama temperature. This is m C H F . in Eqn. (2813).
Constant, Field Function Specifies δ t h as a scalar value.
User Code
Function
Specifies δ t h as a user-defined function.

Material Properties

These material properties can be set for each for each component of film multi-component phases:

Heat of Formation
The heat that is evolved when 1 kilogram of the material is formed from its elements in their respective standard states [J/kg]. See Using the Heat of Formation.
Latent Heat of Vaporization
Available at the component level for multi-component phases.
Method Corresponding Method Node
Enthalpy Difference
Enthalpy Difference
This node provides no properties.
See Using the Enthalpy Difference Method for Latent Heat of Vaporization.
For Simcenter STAR-CCM+ In-cylinder with Fluid Film simulations this property can be specified using a constant scalar profile, field function, Polynomial in T, or Table(T) method.
Saturation Pressure

The saturation pressure p s a t is the pressure of each vapor component when in equilibrium with the corresponding liquid component. This value is required for each liquid component, it can be specified as a Field Function, Polynomial in T, Table (T) or one of the following:

Method Corresponding Method Node
Antoine Equation

Antoine Equation

Defines the saturation pressure using the Antoine equation. See 使用安托因方程.
Wagner Equation

Wagner Equation

Defines the saturation pressure using the Wagner equation. See 使用瓦格纳方程.

Standard State Temperature
The temperature at which the standard state of the material is defined. See 使用标准状态温度.
Critical Temperature
The temperature above which the material cannot be liquefied, regardless of the pressure that is applied. This value is required for each liquid component.
Critical Pressure
The pressure above which liquid and gas cannot coexist at any temperature. This value is required for each liquid component.

These material properties can be set for each fluid film multi-component phase:

Leidenfrost Temperature
The temperature at which the Leidenfrost effect appears. This effect creates a vapor barrier between liquid and solid phases which reduces heat transfer and adhesion. See 使用莱登弗洛斯特温度.
Nukiyama Temperature

Sets the Nukiyama temperature T N also known as the critical heat flux temperature T c r in Eqn. (2825). This is the temperature at which a liquid begins to boil and produces vapor bubbles. The Nukiyama temperature is required for each multi-component liquid.

Method Corresponding Material Properties
Estimated

Estimates the Nukiyama temperature to be halfway between the film saturation temperature and the Leidenfrost temperature according to Eqn. (2826).

None.

Habchi

Use this method if you are expecting pressure variations in your simulation.

Activates the following material properties for each multi-component fluid film phase:
Critical Temperature
Specifies the highest of the critical temperatures of the liquid components. This is T c in Eqn. (2825).
Saturation Temperature
T s a t in Eqn. (2825).
Normal Boiling Temperature
The boiling temperature at standard temperature and pressure conditions. This is T b in Eqn. (2825).
Normal Nukiyama Temperature
The Nukiyama temperature at standard temperature and pressure conditions.

Field Functions

The following field functions are made available when the Boiling Models are activated. These field function are available only on the liquid side.
Film Boiling Latent Heat
The latent heat of phase transfer due to boiling (J/kg).
Film Boiling Latent Heat Flux
The total power (W/m2) that is spent during the phase change due to wall boiling.
Film Boiling Mass Fraction of [component]
The latent heat of phase transfer due to boiling (J/kg).
Film Boiling Rate of [component]
The evaporation rate due to wall boiling (kg/m2-s) for every interacting component.
Film Boiling Temperature
The boiling temperature (K) of the liquid mixture.
Film Bulk Boiling Latent Heat Flux
The total power (W/m2) that is spent during the phase change due to boiling in film cells.
Film Bulk Boiling Rate
The evaporation rate due to boiling inside the film cell (kg/m2-s) for every interacting component.
Wall Boiling Heat Flux of [phase interaction]
The total power (W/m2) that is spent during the phase change due to wall boiling for the phase interaction.
Nukiyama Temperature
The Nukiyama temperature obtained from T c r in Eqn. (2825).