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What is the rigorous limit definition of the divergence of a vector field at a point M?

The divergence of a vector field F⃗\vec{F} at a point MM is defined as the limit of the flux per unit volume as the enclosing volume shrinks to zero around MM. The formula is lim⁡V→01V∬SF⃗⋅n⃗dS=div F⃗(M)\lim_{V \to 0} \frac{1}{V} \iint_S \vec{F} \cdot \vec{n} dS = \text{div } \vec{F}(M).

Conditions

  • The volume VV shrinks to the point MM (radius tends to zero)
  • The vector field F⃗\vec{F} is smooth in the neighborhood of MM

Reasoning, step by step

  1. Consider a small closed surface SS surrounding point MM with enclosed volume VV.
  2. Calculate the flux ∬SF⃗⋅n⃗dS\iint_S \vec{F} \cdot \vec{n} dS.
  3. Normalize by dividing by volume VV.
  4. Take the limit as V→0V \to 0.
  5. The resulting value is the divergence at MM.

Example

The core defining equation appears as: lim⁡V→01V∬SF⃗⋅n⃗dS=div F⃗(M)\lim_{V \to 0} \frac{1}{V} \iint_S \vec{F} \cdot \vec{n} dS = \text{div } \vec{F}(M).

Common misconceptions

  • Assuming the shape of the shrinking volume matters; for smooth fields, the limit is independent of shape.
  • Thinking divergence is only about the boundary; it is a local property derived from the infinitesimal limit.

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