Euler-Lagrange Equation Calculator

Build governing equations from configurable Lagrangian terms fast. Inspect symbolic derivatives, residuals, and acceleration estimates. Use responsive inputs, exports, examples, and clear guidance easily.

Model a customizable Lagrangian, derive partial derivatives, evaluate the Euler–Lagrange residual, and estimate q̈ from the current state.

Calculator Inputs

Large screens show 3 columns, medium screens show 2, and phones show 1.

Used only for symbolic display.

Formula Used

General configurable Lagrangian
L = (a/2)q̇² + (n/4)q̇⁴ + bqq̇ - (c/2)q² - dq - etq + f sin(q) + g cos(q) - hq̇ - (i/4)q⁴ - (j/3)q³ + kt²
Euler–Lagrange equation
d/dt(∂L/∂q̇) - ∂L/∂q = 0
Derived reduced form for this calculator
(a + 3nq̇²)q̈ + cq + d + et - f cos(q) + g sin(q) + iq³ + jq² = 0

This calculator evaluates the partial derivatives numerically at the chosen state and then computes the residual of the Euler–Lagrange equation.

When the effective inertial factor a + 3nq̇² is nonzero, the calculator also solves directly for q̈.

How to Use This Calculator

  1. Enter the coordinate symbol and the coefficients that define your Lagrangian.
  2. Set the current state values q, q̇, q̈, and time t.
  3. Click the solve button to derive the displayed Euler–Lagrange components.
  4. Read the constructed Lagrangian, the partial derivatives, and the reduced governing equation.
  5. Use the residual to test whether the entered state satisfies the equation.
  6. Use the solved q̈ value when the effective inertial factor is not zero.
  7. Export the current output as CSV or PDF for reports or study notes.

Example Data Table

Case a c g i j q t Estimated q̈
Harmonic oscillator 1 4 0 0 0 0.5 0.2 0 -2
Driven linear system 2 6 0 0 0 0.4 0.1 2 -2.2
Cosine potential 1 0 9.81 0 0 0.2 0.0 0 -1.949
Nonlinear polynomial 1 0 0 2 3 1.1 0.6 0 -4.086

FAQs

1. What does this calculator compute?

It builds a configurable one-coordinate Lagrangian, computes ∂L/∂q, ∂L/∂q̇, d/dt(∂L/∂q̇), the Euler–Lagrange residual, and a solved q̈ when the inertial denominator is nonzero.

2. Why does the q·q̇ term often disappear?

For constant coefficient b, the product q·q̇ is a total derivative of q²/2. Total-derivative terms change the action by a boundary contribution and therefore cancel from the Euler–Lagrange equation.

3. Why does a linear q̇ term not change the final equation?

A constant multiple of q̇ is also a total derivative. It shifts the Lagrangian numerically, but it does not alter the governing differential equation for the generalized coordinate.

4. Are the trigonometric inputs in degrees or radians?

They are interpreted in radians. If your source data is in degrees, convert it first by multiplying the angle by π/180 before entering it.

5. What does the residual tell me?

The residual is d/dt(∂L/∂q̇) − ∂L/∂q evaluated at your entered state. A value near zero means the supplied q, q̇, q̈, and t are consistent with the equation.

6. When is the solved q̈ unavailable?

It becomes unavailable when a + 3nq̇² equals zero. In that case, the effective inertial factor vanishes and the equation cannot be solved uniquely for q̈.

7. Can I model nonlinear systems with this tool?

Yes. The q̇⁴, q³, q⁴, sin(q), and cos(q) terms allow you to study nonlinear kinetic and potential effects within the predefined term family.

8. Is this a symbolic algebra engine?

No. It is a structured advanced calculator for a rich predefined Lagrangian family. It derives the matching Euler–Lagrange form and evaluates it numerically from your coefficients and state values.

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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.