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flowBoundaryConditions.js
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/**
* ════════════════════════════════════════════════════════════════
* FEAScript Core Library
* Lightweight Finite Element Simulation in JavaScript
* Version: 0.3.0 (RC) | https://feascript.com
* MIT License © 2023–2026 FEAScript
* ════════════════════════════════════════════════════════════════
*/
// Internal imports
import { basicLog, debugLog, errorLog } from "../utilities/logging.js";
/**
* Class to handle flow boundary conditions application for Stokes and Navier-Stokes models
*/
export class FlowBoundaryConditions {
/**
* Constructor to initialize the FlowBoundaryConditions class
* @param {object} boundaryConditions - Object containing boundary conditions for the finite element analysis
* @param {array} boundaryElements - Array containing elements that belong to each boundary
* @param {array} nop - Nodal numbering (NOP) array representing the connectivity between elements and nodes
* @param {string} meshDimension - The dimension of the mesh (e.g., "2D")
* @param {string} elementOrder - The order of elements (e.g., "linear", "quadratic")
* @param {number} totalNodesVelocity - Total number of velocity nodes (Q2)
* @param {number} totalNodesPressure - Total number of pressure nodes (Q1)
* @param {Map} q2ToPressureMap - Map from global Q2 node index to pressure DOF index
*/
constructor(
boundaryConditions,
boundaryElements,
nop,
meshDimension,
elementOrder,
totalNodesVelocity,
totalNodesPressure,
q2ToPressureMap,
) {
this.boundaryConditions = boundaryConditions;
this.boundaryElements = boundaryElements;
this.nop = nop;
this.meshDimension = meshDimension;
this.elementOrder = elementOrder;
this.totalNodesVelocity = totalNodesVelocity;
this.totalNodesPressure = totalNodesPressure;
this.q2ToPressureMap = q2ToPressureMap;
}
/**
* Function to impose velocity Dirichlet boundary conditions
* @param {array} residualVector - The residual vector to be modified
* @param {array} jacobianMatrix - The Jacobian matrix to be modified
*
* For consistency across both linear and nonlinear formulations,
* this project always refers to the assembled right-hand side vector
* as `residualVector` and the assembled system matrix as `jacobianMatrix`.
*
* In linear problems `jacobianMatrix` is equivalent to the
* classic stiffness/conductivity matrix and `residualVector`
* corresponds to the traditional load (RHS) vector.
*
* Supported boundary condition types:
* - "constantVelocity": Set velocity components at boundary nodes
* Format: ["constantVelocity", uValue, vValue]
* - "stressFree": Natural boundary condition (zero traction), no assembly needed
* Format: ["stressFree"]
*/
imposeDirichletBoundaryConditions(residualVector, jacobianMatrix) {
const totalDOFs = residualVector.length;
let hasStressFree = false;
if (this.meshDimension === "2D") {
Object.keys(this.boundaryConditions).forEach((boundaryKey) => {
const bcType = this.boundaryConditions[boundaryKey][0];
if (bcType === "stressFree") {
hasStressFree = true;
// Natural boundary condition - no explicit assembly needed
debugLog(`Boundary ${boundaryKey}: Applying stress-free condition (natural BC)`);
} else if (bcType === "constantVelocity") {
const uValue = this.boundaryConditions[boundaryKey][1];
const vValue = this.boundaryConditions[boundaryKey][2];
debugLog(
`Boundary ${boundaryKey}: Applying constant velocity condition (u=${uValue}, v=${vValue})`,
);
this.boundaryElements[boundaryKey].forEach(([elementIndex, side]) => {
if (this.elementOrder === "quadratic") {
const boundarySides = {
0: [0, 3, 6], // Nodes at the bottom side of the reference element
1: [0, 1, 2], // Nodes at the left side of the reference element
2: [2, 5, 8], // Nodes at the top side of the reference element
3: [6, 7, 8], // Nodes at the right side of the reference element
};
boundarySides[side].forEach((nodeIndex) => {
const globalNodeIndex = this.nop[elementIndex][nodeIndex] - 1;
const uDOF = globalNodeIndex;
const vDOF = this.totalNodesVelocity + globalNodeIndex;
debugLog(
` - Applied velocity Dirichlet to node ${globalNodeIndex + 1} (element ${
elementIndex + 1
}, local node ${nodeIndex + 1})`,
);
// Apply u-velocity Dirichlet boundary condition
residualVector[uDOF] = uValue;
for (let colIndex = 0; colIndex < totalDOFs; colIndex++) {
jacobianMatrix[uDOF][colIndex] = 0;
}
jacobianMatrix[uDOF][uDOF] = 1;
// Apply v-velocity Dirichlet boundary condition
residualVector[vDOF] = vValue;
for (let colIndex = 0; colIndex < totalDOFs; colIndex++) {
jacobianMatrix[vDOF][colIndex] = 0;
}
jacobianMatrix[vDOF][vDOF] = 1;
});
} else if (this.elementOrder === "linear") {
const boundarySides = {
0: [0, 2], // Nodes at the bottom side of the reference element
1: [0, 1], // Nodes at the left side of the reference element
2: [1, 3], // Nodes at the top side of the reference element
3: [2, 3], // Nodes at the right side of the reference element
};
boundarySides[side].forEach((nodeIndex) => {
const globalNodeIndex = this.nop[elementIndex][nodeIndex] - 1;
const uDOF = globalNodeIndex;
const vDOF = this.totalNodesVelocity + globalNodeIndex;
debugLog(
` - Applied velocity Dirichlet to node ${globalNodeIndex + 1} (element ${
elementIndex + 1
}, local node ${nodeIndex + 1})`,
);
// Apply u-velocity Dirichlet boundary condition
residualVector[uDOF] = uValue;
for (let colIndex = 0; colIndex < totalDOFs; colIndex++) {
jacobianMatrix[uDOF][colIndex] = 0;
}
jacobianMatrix[uDOF][uDOF] = 1;
// Apply v-velocity Dirichlet boundary condition
residualVector[vDOF] = vValue;
for (let colIndex = 0; colIndex < totalDOFs; colIndex++) {
jacobianMatrix[vDOF][colIndex] = 0;
}
jacobianMatrix[vDOF][vDOF] = 1;
});
}
});
}
});
// If no stress-free boundary exists, pin pressure at one node to remove null space
// (pressure is determined only up to a constant for all-Dirichlet velocity problems)
if (!hasStressFree) {
const pDOF = 2 * this.totalNodesVelocity; // First pressure DOF
for (let colIndex = 0; colIndex < totalDOFs; colIndex++) {
jacobianMatrix[pDOF][colIndex] = 0;
}
jacobianMatrix[pDOF][pDOF] = 1;
residualVector[pDOF] = 0;
debugLog("Pinned pressure at first pressure node (p = 0) to remove null space");
}
}
}
}