1 r ⋅ ∂ ∂ r [ r ( μ ∂ v z ∂ r ) ] − ∂ p ∂ z = ∂ ( ρ v z ) ∂ t ∂ ρ ∂ t + v z ∂ ρ ∂ z = − ρ ∂ v z ∂ z = 0
1 r d E z d r + d 2 E z d r 2 + k 2 E z = 0 alternatively 1 r d E θ d r + d 2 E θ d r 2 − E θ r 2 + k 2 E θ = 0
E z = A z ∗ J 0 ( k ⋅ r ) + B z ∗ Y 0 ( k ⋅ r ) alternatively E θ = A θ ∗ J 1 ( k ⋅ r ) + B θ ∗ Y 1 ( k ⋅ r )
− v z ( r ) ∂ C A ∂ z + ∂ ∂ z ( D ∂ C A ∂ z ) + 1 r ∂ ∂ r [ r ( D ∂ C A ∂ r ) ] − ( − r A ) = ∂ C A ∂ t
− v z ( r ) ∂ ( ρ c p T ) ∂ z + ∂ ∂ z ( K ∂ T ∂ z ) + 1 r ∂ ∂ r [ r ( K ∂ T ∂ r ) ] + ( − r A ) ( − Δ H r ) + { π f ε 0 ε ″ | E z | 2 π f ε 0 ε ″ | E θ | 2 = ρ c p ∂ T ∂ t
− r A = ( − r A ) max C A C B C A C B + k B C A ( 1 + C A k i A ) + k A C B ( 1 + C B k i B )
t = 0
v z = 0
C A = 0
∀ r , ∀ z
r = 0
∂ v z ∂ r = 0
∂ C A ∂ r = 0
∂ T ∂ r = 0
d E z d r = 0
alternatively
d E θ d r = 0
∀ z , ∀ t > 0
r = R
E z = E z 0
E θ = E θ 0
z = 0
p = p 0
C A = C A 0
T = T 0
∀ r , ∀ t > 0
z = L
p = p L
∂ C A ∂ z = 0
∂ T ∂ z = 0