2.2. Blade Element Theory Model

2.2.1. Overview

Based on Blade Element Theory, Flow360 provides 2 related solvers, which can be configured in BETDisks section of Flow360.json:

  • Steady blade disk solver

    To use the steady blade disk solver, the bladeLineChord needs to be set as 0, which is its default value if omitted.

  • Unsteady blade line solver

    To use the unsteady blade line solver, bladeLineChord has to be a positive value and initialBladeDirection also needs to be set.

In the BETDisks section of the Flow360.json, except the bladeLineChord and initialBladeDirection, other parameters are necessary for both solvers. A case study on the XV-15 rotor using blade element theory can be found at XV15 BET Disk.

2.2.2. BET input

Note

  1. In the BETDisks section, all input quantities are non-dimensional, except the twists and alphas (both in degrees). The convention for non-dimensionalization in Flow360 can be found at Non-dimensionalization in Flow360.

  2. For users of XROTOR and DFDC, we have a translator script that will convert the XROTOR/DFDC inputs in Flow360 BET inputs.

Some input parameters related to BET solver in Flow360 are explained:

  1. radius. All grid points enclosed by the cylinder defined by “radius”, “center” and “axisOfRotation” will have aerodynamic forces imposed on them according to blade element theory.

  2. rotationDirectionRule: leftHand or rightHand. It depends on the design of the rotor blades: whether the blades follow curl left hand rule or the curl right hand rule to generate positive thrust. The following 2 figures show the curl left hand rule and curl right hand rule. The fingers follow the spinning of the blades and the thumb points to the thrust direction. By default, it is rightHand.

../_images/left_hand_rule.svg
../_images/right_hand_rule.svg

  1. axisOfRotation: It is the direction of your thumb (thrust) described in “rotationDirectionRule”.

  2. omega: The non-dimensional rotating speed. It should be positive in most cases, which means the leading edge moves in front and the rotation direction of the blades in BET simulations is consistent with the curling fingers described in “rotationDirectionRule” to generate positive thrust. A negative “omega” means the blades rotate in a reverse direction, where the trailing edge moves in front.

The following 4 pictures give some examples of different rotationDirectionRule and axisOfRotation with positive omega. The curved arrow follows the same direction in which rotor spins. The straight arrow points to the direction of thrust.

"rotationDirectionRule":"leftHand",
"axisOfRotation":[0,0,1],
"omega": 0.3
../_images/leftHand_thrust_z+.svg 
"rotationDirectionRule":"leftHand",
"axisOfRotation":[0,0,-1],
"omega": 0.5
../_images/leftHand_thrust_z-.svg 
"rotationDirectionRule":"rightHand",
"axisOfRotation":[0,0,1],
"omega": 0.5
../_images/rightHand_thrust_z+.svg 
"rotationDirectionRule":"rightHand",
"axisOfRotation":[0,0,-1],
"omega": 0.5
../_images/rightHand_thrust_z-.svg

Note

In the above 4 examples, if the omega is negative, the rotor rotates in the opposite direction of what is shown.

  1. chords and twists: The sampled radial distribution of chord length and twist angle. The “twist” affects the local angle of attack. The “chords” affects the amount of lift and drag imposed on the blade (or fluid). For a radial location where chord=0, there is no lift or drag imposed. It should be noted that for any radial location within the given sampling range, the chord or twist is linearly interpolated between its two neighboring sampled data points. For any radial location beyond the given sampling range, the chord or twist is set to be the nearest sampled chord or twist, i.e. constant extrapolation. Here are 3 examples of the given “chords” and the corresponding radial distribution of chord length:

5.1. The root of blade starts at r=20 with chord length=15. The chord shrinks to 10 linearly up to r=60. The chord keeps as 10 for the rest of blade. In this setting, the chord=0 for r in [0,20], there is no aerodynamic lift and drag imposed no matter what the twist angle it has, so this setting fits the rotor without hub.

[
    {
        "radius": 19.9999,
        "chord": 0
    },
    {
        "radius": 20,
        "chord": 15
    },
    {
        "radius": 60,
        "chord": 10
    },
    {
        "radius": 150,
        "chord": 10
    }
]
../_images/chords_distribution_1.svg

5.2. The root of blade starts at r=0 with chord=0. The chord expands to 15 linearly up to r=20, then shrinks to 10 linearly up to r=60. The chord keeps as 10 for the rest of blade. This setting could be used for a mesh with the geometry of hub. Because the chord length changes gradually near the root region, there won’t be tip vortices in root region.

[
    {
        "radius": 0,
        "chord": 0
    },
    {
        "radius": 20,
        "chord": 15
    },
    {
        "radius": 60,
        "chord": 10
    },
    {
        "radius": 150,
        "chord": 10
    }
]
../_images/chords_distribution_2.svg

5.3. This is an exmpale of wrong setting of chords, because the chord length at r=0 is not 0, so the local solidity is infinity, which is not realistic.

[
    {
        "radius": 20,
        "chord": 15
    },
    {
        "radius": 60,
        "chord": 10
    },
    {
        "radius": 150,
        "chord": 10
    }
]
../_images/chords_distribution_3.svg

Note

The number of sampling data points in chords and twists doesn’t have to be the same. They are served as sampled data for interpolation of chord length and twist angle respectively and separately.

2.2.3. BET Loading Output

After the simulation is completed, a “bet_forces_v2.csv” file is created for the case, which contains the time history of the following quantities:

  1. Integrated x-, y-, z-component of non-dimensional forces and non-dimensional moments acted on each disk, represented by “Disk[diskID]_Force_x,_y,_z” and “Disk[diskID]_Moment_x,_y,_z” in the “bet_forces_v2.csv file” respectively. The non-dimensional force is defined as

(2.2.1)\[\text{Force}_\text{non-dimensional} = \frac{\text{Force}_\text{physical}\text{(SI=N)}}{\rho_\infty C_\infty^2 L_{gridUnit}^2}\]

The non-dimensional moment is defined as

(2.2.2)\[\text{Moment}_\text{non-dimensional} = \frac{\text{Moment}_\text{physical}\text{(SI=N$\cdot$m)}}{\rho_\infty C_\infty^2 L_{gridUnit}^3},\]

where the moment center is the centerOfRotation of each disk, defined in BETDisks of Flow360.json.

Note

The above Force and Moment values mean the force and moment acted on solid. If you want to know the force and moment acted on fluid, just add a negative sign in front of it.

  1. Sectional thrust coefficient \(C_t\) and sectional torque coefficient \(C_q\) on each blade at several radial locations, represented by “Disk[diskID]_Blade[bladeID]_R[radialID]” with suffix “_Radius” (non-dimensional), “_ThrustCoeff” and “_TorqueCoeff”. The number of radial locations is specified in nLoadingNodes.

The definition of \(C_t\) is

(2.2.3)\[C_t\bigl(r\bigr)=\frac{\text{Thrust per unit blade span (SI=N/m)}}{\frac{1}{2}\rho_{\infty}\left((\Omega r)^2\right)\text{chord}_{\text{ref}}}\cdot\frac{r}{R}\]

The definition of \(C_q\) is

(2.2.4)\[C_q\bigl(r\bigr)=\frac{\text{Torque per unit blade span (SI=N)}}{\frac{1}{2}\rho_{\infty}\left((\Omega r)^2\right)\text{chord}_{\text{ref}}R}\cdot\frac{r}{R}\]

where \(r\) is the dimensional distance between the node to the axis of rotation. \(\text{chord}_\text{ref}\) is the dimensional reference chord length. \(R\) is the dimensional radius of the rotor disk.

Important

All the quantities in the right hand side of Eq.(2.2.1), Eq.(2.2.2), Eq.(2.2.3) and Eq.(2.2.4) are dimensional, which are different from the non-dimensional values in BETDisks (list) of Flow360.json. For example, at the first disk’s first blade’s first radial location \(r=\text{Disk0_Blade0_R0_Radius}\times L_\text{gridUnit}\). The conventions for non-dimensionalization in Flow360 can be found at Non-dimensionalization in Flow360.

Warning

For simulations of the steady blade disk solver, the resulting \(C_t\) and \(C_q\) are only saved on the first blade, named by “Blade0”. They are written as all zeros for other blades, because all the blades have the same sectional loadings in steady blade disk simulations. For the unsteady blade line solver, each blade has its own \(C_t\) and \(C_q\) values.

Here is an example of the header of a “bet_forces_v2.csv” file from a simulation containing two BET disks (assume nLoadingNodes = 20, numberOfBlades = 3 for each disk):

physical_step, pseudo_step,
Disk0_Force_x, Disk0_Force_y, Disk0_Force_z, Disk0_Moment_x, Disk0_Moment_y, Disk0_Moment_z,
Disk0_Blade0_R0_Radius, Disk0_Blade0_R0_ThrustCoeff, Disk0_Blade0_R0_TorqueCoeff,
Disk0_Blade0_R1_Radius, Disk0_Blade0_R1_ThrustCoeff, Disk0_Blade0_R1_TorqueCoeff,
...
Disk0_Blade0_R19_Radius, Disk0_Blade0_R19_ThrustCoeff, Disk0_Blade0_R19_TorqueCoeff,
Disk0_Blade1_R0_Radius, Disk0_Blade1_R0_ThrustCoeff, Disk0_Blade1_R0_TorqueCoeff,
Disk0_Blade1_R1_Radius, Disk0_Blade1_R1_ThrustCoeff, Disk0_Blade1_R1_TorqueCoeff,
...
Disk0_Blade1_R19_Radius, Disk0_Blade1_R19_ThrustCoeff, Disk0_Blade1_R19_TorqueCoeff,
Disk0_Blade2_R0_Radius, Disk0_Blade2_R0_ThrustCoeff, Disk0_Blade2_R0_TorqueCoeff,
Disk0_Blade2_R1_Radius, Disk0_Blade2_R1_ThrustCoeff, Disk0_Blade2_R1_TorqueCoeff,
...
Disk0_Blade2_R19_Radius, Disk0_Blade2_R19_ThrustCoeff, Disk0_Blade2_R19_TorqueCoeff,
Disk1_Force_x, Disk1_Force_y, Disk1_Force_z, Disk1_Moment_x, Disk1_Moment_y, Disk1_Moment_z,
...
...
...
Disk1_Blade2_R19_Radius, Disk1_Blade2_R19_ThrustCoeff, Disk1_Blade2_R19_TorqueCoeff

2.2.4. BET Visualization

An additional option betMetrics in volumeOutput is available to visualize the BET related quantities.

Note

A case study about the XV-15 rotor using steady BET Disk solver can be found at XV15 BET Disk case.