Gauss divergence theorems
1. Statement — Gauss Divergence Theorem (Ostrogradsky)
Let be a bounded, closed, piecewise smooth solid with outward oriented closed surface . If has continuous first partials on an open region containing , then:
i.e. total outward flux = volume integral of divergence (source density integrated). means closed surface.
2. Geometric Meaning
Integrate source density over volume ⇒ net flux out. If inside, more exits than enters (source); if , net flux zero (solenoidal, what goes in comes out).
3. Working Steps (recipe)
- Compute (often constant/simple).
- Describe (Cartesian/cylindrical/spherical) and evaluate (often far easier than surface integral).
- That value equals .
Conversely, to find volume integral of divergence, compute flux — whichever easier.
4. Worked Examples
(a) F= r = x i+y j+z k, V: ball x²+y²+z²≤a²: ∇·F=3 ⇒ ∯_{S}F·n dS =∭_{V}3 dV =3·4πa³/3=4πa³ ✓ matches earlier direct flux a·area.
(b) F= x² i+ y² j+ z² k, V: cube 0≤x,y,z≤1: ∇·F=2x+2y+2z ⇒ ∭=∫_{0}^{1}∫_{0}^{1}∫_{0}^{1}(2x+2y+2z)dz dy dx =3 ✓
Direct flux through 6 faces sums to same but longer.
(c) F= -y i+ x j ??? Need divergence zero ⇒ flux zero for any closed surface not enclosing singularity? Check.
(d) F= r/r³ , r≠0: ∇·F=0 except at origin ⇒ ∯_{sphere}F·n dS=4π (point source) but ∭_{V}0=0 if origin excluded? Shows need to handle singularity — Gauss fails if singularity inside, need punctured volume.
(e) Electrostatics: F=E= q r/(4π ε₀ r³) ⇒ ∇·E=0 away from charge, but ∯ E·n dS = q/ε₀ via singularity — Gauss's law.
5. Relation to Green (2D)
Flux form of Green in plane is 2D Gauss: .
6. Exam Points
- State Gauss divergence theorem with outward — 3-5 marks, almost certain.
- Evaluate via for sphere/cube/cylinder — 7-10 marks, very frequent (often "using Gauss" compulsory).
- Show for but flux =4π — 5 marks, frequent (handling singularity).
- Volume via or vice versa — 5 marks.