Curl Calculator
Calculate the curl of any 2D or 3D vector field with a step-by-step determinant expansion. Enter the component functions, get the symbolic curl, evaluate it at a point, spot irrotational fields and view a vorticity overlay.
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About Curl Calculator
The Curl Calculator computes the curl ∇×F of any 2D or 3D vector field with full step-by-step cross product determinant expansion. Enter your vector field components P, Q (and R for 3D), optionally evaluate at a specific point, and get the symbolic curl, rotation classification, and for 2D fields, an interactive visualization with a vorticity heat map and animated particle flow showing the rotational behavior of the field.
What Is Curl?
The curl of a vector field \(\mathbf{F}\) measures the infinitesimal rotation of the field at each point. For a 3D field \(\mathbf{F} = \langle P, Q, R \rangle\), the curl is computed as a cross product:
$$\nabla \times \mathbf{F} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\ P & Q & R \end{vmatrix}$$
Expanding the determinant gives the curl vector:
$$\nabla \times \mathbf{F} = \left\langle \frac{\partial R}{\partial y} - \frac{\partial Q}{\partial z},\; \frac{\partial P}{\partial z} - \frac{\partial R}{\partial x},\; \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right\rangle$$
For a 2D field \(\mathbf{F} = \langle P, Q \rangle\), the curl reduces to the scalar \(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\), which represents rotation in the xy-plane.
Physical Meaning of Curl
Curl Formulas in Different Coordinate Systems
| Coordinate System | Curl Formula |
|---|---|
| Cartesian 2D | \(\text{curl}\,\mathbf{F} = \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\) (scalar) |
| Cartesian 3D | \(\nabla \times \mathbf{F} = \left\langle \frac{\partial R}{\partial y} - \frac{\partial Q}{\partial z},\; \frac{\partial P}{\partial z} - \frac{\partial R}{\partial x},\; \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right\rangle\) |
| Cylindrical | \(\nabla \times \mathbf{F} = \left\langle \frac{1}{r}\frac{\partial F_z}{\partial \theta} - \frac{\partial F_\theta}{\partial z},\; \frac{\partial F_r}{\partial z} - \frac{\partial F_z}{\partial r},\; \frac{1}{r}\frac{\partial(rF_\theta)}{\partial r} - \frac{1}{r}\frac{\partial F_r}{\partial \theta} \right\rangle\) |
| Spherical | See full expansion using scale factors \(h_r=1, h_\theta=r, h_\phi=r\sin\theta\) |
Important Identities Involving Curl
| Identity | Formula |
|---|---|
| Curl of gradient | \(\nabla \times (\nabla f) = \mathbf{0}\) (always zero — gradients are irrotational) |
| Divergence of curl | \(\nabla \cdot (\nabla \times \mathbf{F}) = 0\) (always zero — curls are solenoidal) |
| Linearity | \(\nabla \times (a\mathbf{F} + b\mathbf{G}) = a(\nabla \times \mathbf{F}) + b(\nabla \times \mathbf{G})\) |
| Product rule | \(\nabla \times (f\mathbf{F}) = f(\nabla \times \mathbf{F}) + (\nabla f) \times \mathbf{F}\) |
| Stokes' theorem | \(\displaystyle\iint_S (\nabla \times \mathbf{F}) \cdot d\mathbf{S} = \oint_C \mathbf{F} \cdot d\mathbf{r}\) |
Applications of Curl
| Field | Application | What Curl Represents |
|---|---|---|
| Electromagnetism | Faraday's Law | \(\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}\) — changing magnetic fields create circulating electric fields |
| Electromagnetism | Ampere's Law | \(\nabla \times \mathbf{B} = \mu_0 \mathbf{J}\) — electric currents create circulating magnetic fields |
| Fluid Dynamics | Vorticity | \(\boldsymbol{\omega} = \nabla \times \mathbf{v}\) — measures how the fluid spins locally |
| Mechanics | Angular velocity | For rigid body rotation \(\mathbf{v} = \boldsymbol{\omega} \times \mathbf{r}\), the curl gives \(2\boldsymbol{\omega}\) |
| Conservative fields | Path independence | If \(\nabla \times \mathbf{F} = 0\), line integrals are path-independent and a potential exists |
How to Use the Curl Calculator
- Choose dimension: Select 2D for fields F = ⟨P, Q⟩ (scalar curl) or 3D for F = ⟨P, Q, R⟩ (vector curl) using the toggle buttons.
- Enter component functions: Type each component function (P, Q, and optionally R) using standard notation. Use
^for exponents,*for multiplication, and functions likesin(x),cos(y),exp(x),ln(x),sqrt(x). Implicit multiplication is supported (e.g.,2x=2*x). - Enter an evaluation point (optional): Provide comma-separated coordinates to evaluate the curl numerically and classify the rotation direction.
- Click Compute Curl: View the symbolic curl, step-by-step cross product determinant expansion, numerical evaluation, and rotation classification.
- Explore the visualization: For 2D fields, view the vector field arrows with a vorticity heat map (orange = counterclockwise, purple = clockwise) and animated particle flow.
Worked Example
Find the curl of \(\mathbf{F}(x, y, z) = \langle y z,\; x z,\; x y \rangle\) at the point \((1, 2, 3)\):
Step 1: Write the determinant: \(\nabla \times \mathbf{F} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ \partial_x & \partial_y & \partial_z \\ yz & xz & xy \end{vmatrix}\)
Step 2: Expand: \(\mathbf{i}(x - x) - \mathbf{j}(y - y) + \mathbf{k}(z - z) = \langle 0, 0, 0 \rangle\)
Step 3: The curl is identically zero — this field is irrotational (conservative). In fact, \(\mathbf{F} = \nabla(xyz)\), confirming a potential function exists.
Curl vs. Divergence
| Property | Curl (∇×F) | Divergence (∇·F) |
|---|---|---|
| Operator type | Cross product with ∇ | Dot product with ∇ |
| Output | Vector (3D) / Scalar (2D) | Scalar |
| Measures | Rotation / circulation | Expansion / contraction |
| Zero means | Irrotational / conservative | Solenoidal / incompressible |
| Theorem | Stokes' theorem | Divergence (Gauss) theorem |
FAQ
Reference this content, page, or tool as:
"Curl Calculator" at https://MiniWebtool.com/curl-calculator/ from MiniWebtool, https://MiniWebtool.com/
by miniwebtool team. Updated: 2026-04-08
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