The curl ∇ × F measures rotation and circulation of F; for F = ⟨P, Q, R⟩, curl F = ⟨(∂R/∂y − ∂Q/∂z), (∂P/∂z − ∂R/∂x), (∂Q/∂x − ∂P/∂y)⟩. The divergence ∇ · F = ∂P/∂x + ∂Q/∂y + ∂R/∂z measures net outflow. Both are fundamental to Green's, Stokes', and divergence theorems.
Curl and divergence are the two fundamental ways to differentiate a vector field, and each captures a physically distinct property. Divergence asks: is fluid (or field) flowing out from a point, or converging into it? Curl asks: is the fluid spinning, and in which direction? Together they give a complete local picture of how a vector field behaves near any point.
Divergence is the simpler of the two. For F = ⟨P, Q, R⟩, the divergence is just ∇ · F = ∂P/∂x + ∂Q/∂y + ∂R/∂z — a scalar sum of how much each component is "spreading out" along its own axis. Positive divergence at a point means the field expands outward (a source); negative means it contracts inward (a sink). A field with zero divergence everywhere is called solenoidal or incompressible — magnetic fields and incompressible fluid velocity fields satisfy this.
Curl is more complex because it measures rotation, which is inherently a higher-dimensional concept. In 3D, curl F = ∇ × F is a vector (computed like a cross product with ∇ as one factor) that points along the axis of rotation by the right-hand rule. Its magnitude is the strength of the rotation. In 2D, the curl reduces to a single scalar — ∂Q/∂x − ∂P/∂y — which tells you whether field lines swirl counterclockwise (positive) or clockwise (negative). A field with zero curl everywhere is called irrotational, and on a simply connected domain, irrotational is equivalent to being conservative (having a potential function).
The key to not confusing curl and divergence is to remember their symbolic forms: divergence uses ∇ · F (dot product, mixes each component with its own axis), while curl uses ∇ × F (cross product, mixes components with *other* axes). This cross-mixing is exactly what detects rotation. The divergence theorem connects divergence to flux through a closed surface; Stokes' theorem connects curl to circulation around a closed curve — these theorems are where the physical meaning of curl and divergence is most powerfully expressed.