6. Integral Theorems of Vector Calculus Flashcards
Integral Definition of Divergence
Equation
|∇ . |F = (𝛿V->0) lim 1/𝛿V ∯|F . d|S
-where 𝛿S is the surface enclosing the volume 𝛿V with outward normal
Integral Definition of Divergence
Derivation
-take 𝛿V to be the volume of a cuboid of sides 𝛿x 𝛿y 𝛿z centred on the point |x=(x,y,z)
-on face S1 (left face in x direction) |n=(1,0,0) so:
|F.|n = F1(x + 𝛿x/2, y, z)
-on face S2 (right face in x direction, |n=(-1,0,0) so:
|F.|n = -F1(x - 𝛿x/2, y, z)
-hence:
(S1) ∬|F.|n dS = F1(x+𝛿x/2, y, z) 𝛿y 𝛿z
(S2) ∬|F.|n dS = -F1(x-𝛿x/2, y, z) 𝛿y 𝛿z
-Thus:
(S1∪S2)∬|F.|n dS = [F1(x+𝛿x/2, y, z)-F1(x-𝛿x/2,y,z) / 𝛿x] 𝛿x 𝛿y 𝛿z
-so:
(𝛿x->0) lim ∬|F.|n dS = ∂F1/∂x 𝛿V
-simirlarly for the other four faces, so:
(𝛿x,𝛿y,𝛿z ->0) lim ∬|F.|n dS =
(∂F1/∂x + ∂F2/∂y + ∂F3/∂z)𝛿V
-so:
|∇ . |F = (𝛿V->0) lim 1/𝛿V ∯|F . d|S
Integral Definition of Divergence
Description
-the divergence of a vector field |F is equal to the flux of |F out of 𝛿V divided by the volume of 𝛿V
Divergence Theorem
Equation
∯|F . d|S = ∭ (|∇ . |F) dV
Divergence Theorem
Description
-if V is a volume enclosed by a surface S and |F is a continuously differentiable vector field in V, then the divergence theorem states that the flux through that closed surface S is equal to the sum of the divergence at every point within the volume V.
Divergence Theorem
Derivation
Applications of Divergence Theorem
- divergence theorem allows surface integrals (which are often difficult) to be replaced by volume integrals, which are easier
- REMEMBER - we must check every time that the surface is closed, as divergence theorem only applies to closed surfaces
Green’s First Identity
Equation
∭[ (|∇f) . (|∇g) + ∇²g ] dV = ∯ f|∇g . d|S
Green’s First Identity
Derivation
-start with a vector field of the form |F = f |∇g, where f and g are scalar fields
-find the divergence by converting to index notation, rearranging (use product rule) and converting back to vector notation:
|∇ . |F = (|∇f) . (|∇g) + ∇²g
-hence the divergence theorem states that:
∭[ (|∇f) . (|∇g) + ∇²g ] dV = ∯ f|∇g . d|S
Green’s Second Identity
Equation
∭[ f ∇²g - g ∇²f ] dV = ∯ ( f |∇g - g |∇f ) . d|S
Green’s First Identity
Description
-the divergence theorem applied to a vector field of the form |F = f |∇g , where f and g are scalar fields
Another Integral Theorem
Description
-the divergence theorem applied to a vector field of the form |F = |a f , where f is a scalar field and |a is a constant vector
Another Integral Theorem
Derivation
-start with a vector field of the form |F = |a f, where f is a scalar field and |a is a constant vector
-find the divergence by converting to index notation, switching order of variables and converting back to vector notation:
|∇ . |F = |a . (|∇f)
-substitute into the divergence theorem, and cancel |a . from both sides since |a can be taken as any vector if we take |e1, |e2 and |e3 it is clear all components are equal so both vectors must be equal:
∭ |∇f dV = ∯ f d|S
Another Integral Theorem
Equation
∭ |∇f dV = ∯ f d|S
Green’s Second Identity
Description
-the divergence theorem applied to a vector field of the form, |F = f |∇g - g |∇f , where f and g are both scalar fields