Finite Volume Method Solver Calculator

Analyze steady diffusion on uniform grids with clear inputs. Review coefficients, sources, boundaries, and convergence. Download tables, print reports, and visualize node behavior instantly.

Solver Inputs

This page keeps a single-column flow. The calculator fields below use a responsive three, two, and one-column arrangement.

Name your scenario for exported reports.
Examples: Temperature, Potential, Concentration.
Examples: K, V, kg/m³, mol/m³.
Total one-dimensional physical length.
Higher N improves spatial resolution.
Used in diffusion conductance and source volume.
Thermal conductivity or equivalent diffusion coefficient.
Constant source contribution inside each cell.
Usually zero or negative for stable linearization.
Dirichlet condition at x = 0.
Dirichlet condition at x = L.
Controls printed precision in tables and exports.

Formula Used

This solver handles the steady one-dimensional diffusion equation with a linearized source term over uniform control volumes.

d/dx ( Γ A dφ/dx ) + A(Su + Spφ) = 0

For each interior control volume, the algebraic finite-volume form is:

aP φP = aW φW + aE φE + b

The boundary cells use half-cell distances, so each Dirichlet boundary contributes 2De to the source and diagonal coefficient.

The resulting tridiagonal system is solved by the Thomas algorithm, also called TDMA.

How to Use This Calculator

  1. Enter a case label and choose the scalar name.
  2. Set the domain length, number of control volumes, and area.
  3. Enter the diffusion coefficient Γ for your physics problem.
  4. Add source terms Su and Sp if generation or sink exists.
  5. Specify the left and right boundary values.
  6. Choose the displayed decimal precision.
  7. Click Solve with FVM to compute the field.
  8. Review the summary cards, graph, and nodewise table.
  9. Download CSV for spreadsheets or PDF for reporting.

Example Data Table

Example case: L = 1, N = 6, A = 1, Γ = 1.2, Su = 0, Sp = 0, left = 100, right = 200.

Node x Example Field Interpretation
10.0833108.3333Near the left boundary.
20.2500125.0000Linear rise continues.
30.4167141.6667Mid-domain value.
40.5833158.3333Symmetric linear trend.
50.7500175.0000Approaches right boundary.
60.9167191.6667Last cell center value.

FAQs

1) What equation does this solver handle?

It solves the steady one-dimensional diffusion equation with a linearized source term. This covers simplified heat conduction, scalar transport, electric potential, and similar physics models on a uniform grid.

2) What do Su and Sp represent?

Su is the constant source term per unit volume. Sp multiplies the local scalar value. Together they model generation, absorption, or linearized physics contributions inside each control volume.

3) Why is a negative Sp often recommended?

A non-positive Sp usually strengthens diagonal dominance in the algebraic system. That improves stability and keeps the resulting matrix better behaved for diffusion-dominated steady problems.

4) Why does the solver use a uniform grid?

A uniform mesh keeps the formulation transparent and easy to verify. It is ideal for learning, quick estimates, and many smooth one-dimensional problems without geometric stretching.

5) What do the residuals show?

Residuals measure how closely each control-volume equation is balanced after solving. Values near zero mean the discrete conservation equations are satisfied well at that node.

6) Can I use this for temperature, concentration, or voltage?

Yes. The variable is written as a generic scalar φ. You can interpret it as temperature, concentration, potential, or another diffusing quantity.

7) Does this model transient behavior?

No. This page solves steady-state conditions only. Time-dependent diffusion would need an added transient storage term and time-marching scheme.

8) When should I increase the number of control volumes?

Use more cells when gradients are steep, source terms are strong, or you need smoother plots. Grid refinement also helps confirm that the solution is mesh independent.

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Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.