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Finite Element Method for Gravitational Potential Equation

Project Overview

This project implements the Finite Element Method (FEM) to solve the gravitational potential differential equation:

d²Φ/dx² = 4πGρ(x)

with boundary conditions:

  • Φ(0) = 5
  • Φ(3) = 4

and density function:

  • ρ(x) = 0 for x ∈ [0,1]
  • ρ(x) = 1 for x ∈ (1,2]
  • ρ(x) = 0 for x ∈ (2,3]

Project Structure

Files:

  • wyprowadzenie.pdf - Mathematical derivation of the variational formulation and FEM implementation
  • fem.m - MATLAB implementation of the FEM solver

Mathematical Background

Weak Formulation

The strong form is converted to weak formulation using:

  • Test functions v ∈ V that vanish at boundaries
  • Integration by parts to reduce derivative order
  • Construction of bilinear form B(Φ, v) and linear functional L(v)

Shift Function

Due to non-homogeneous Dirichlet boundary conditions, a shift function is introduced: Φ(x) = w(x) + Φ̃(x) where Φ̃(x) = -1/3*x + 5 satisfies the boundary conditions.

Finite Element Discretization

  • Domain Ω = [0,3] divided into N equal elements
  • Linear basis functions e_i(x) with compact support
  • Piecewise linear approximation of the solution

Usage

Parameters:

  • N = 1000 - Number of elements (adjustable)
  • G = 6.6743e-11 - Gravitational constant (adjustable)

Running the Code:

% Simply run the fem.m file in MATLAB
% The code will:
% 1. Set up the finite element discretization
% 2. Assemble the stiffness matrix and load vector
% 3. Solve the linear system
% 4. Plot the solution Φ(x)

Output:

  • Graphical plot of the gravitational potential Φ(x) over domain [0,3]
  • Numerical solution values stored in variable y

Requirements

  • MATLAB
  • No additional toolboxes required

Features

  • Adjustable number of elements N
  • Configurable gravitational constant G
  • Numerical integration using Gauss-Legendre quadrature
  • Automatic handling of non-homogeneous boundary conditions
  • Visualization of the solution

Numerical Method

  • Method: Finite Element Method (FEM)
  • Element Type: Linear Lagrangian elements
  • Integration: 2-point Gauss-Legendre quadrature
  • Matrix Solver: MATLAB's backslash operator (direct solver)

This implementation demonstrates the complete FEM workflow from mathematical formulation to numerical solution for a second-order boundary value problem with piecewise constant coefficients.