Source: \(\vec F = \dfrac{Q}{2\pi}\dfrac{\hat r}{r}\)
Free vortex: \(\vec F = \dfrac{Q}{2\pi}\dfrac{\hat\phi}{r}\)
Saddle: \(\vec F = (Qx, -Qy)\)
Divergence \(\nabla\cdot\vec F\) and curl \(\nabla\times\vec F\) classify the field topology.
Switch between canonical 2D fields — uniform flow, point source, free vortex, dipole and saddle — and adjust strength and arrow density. Click on the canvas to drop streamline seeds; double-click to clear.
Source: \(\vec F = \dfrac{Q}{2\pi}\dfrac{\hat r}{r}\)
Free vortex: \(\vec F = \dfrac{Q}{2\pi}\dfrac{\hat\phi}{r}\)
Saddle: \(\vec F = (Qx, -Qy)\)
Divergence \(\nabla\cdot\vec F\) and curl \(\nabla\times\vec F\) classify the field topology.
A 2D vector field assigns a vector $\vec F(x,y)$ to every point. The simulator visualises it three ways: discrete arrows on a grid, integrated streamlines, and an optional magnitude colormap. The streamlines are obtained by integrating $\dot{\vec r}=\vec F/|\vec F|$ with a fixed step.
Two scalar quantities classify the field. Divergence $\nabla\cdot\vec F = \partial_x u + \partial_y v$ measures local outflow; curl $\nabla\times\vec F = \partial_x v - \partial_y u$ measures local rotation. The cursor probe estimates these numerically by central differences.
Aerodynamics: potential-flow combinations of uniform, source, dipole and vortex elements model lift and bluff-body flow before viscous CFD is run.
Electromagnetism: the same equations describe 2D electrostatic and magnetostatic fields. Source = positive charge, dipole = electric dipole, vortex = magnetic field of a long wire.
Dynamical systems: phase-plane analysis of ODE systems uses exactly this kind of arrow plot to diagnose fixed-point stability.