Advanced Applied Mathematical Analysis Homework in Chemical Engineering, Assignments of Chemistry

The ninth homework assignment for the course che 527: advanced applied mathematical analysis in chemical engineering, which was due in class on november 21, 2006. The assignment includes four problems related to potential flow past a sphere, diffusive mass transfer in a liquid drop, the wave equation, and motion of a mass on a spring with damping.

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CHE 527 Advanced Applied Mathematical Analysis in Chemical Engineering Fall 2006
Homework 9
Due in class on Tuesday, November 21.
1. Potential flow past a sphere is governed by
2φ=1
r2
∂r r2φ
∂r +1
r2sin θ
∂θ sin θφ
∂θ = 0
where
v=φ=∂φ
∂r er+1
r
∂φ
∂θ eθ
is the velocity. Use separation of variables to solve for φ(r, θ) in the domain ar subject to the
B.C.’s ∂φ
∂r = 0 on r=a, and ∂φ
∂r =Ucos θas r .
2. Consider the diffusive mass transfer (2c= 0) of a solute inside a liquid drop subject to a mass transfer
boundary condition (−D ∂c
∂r =k(cc0) at r=a). For an axisymmetric case c0=c1+c2cos θ, where
c1and c2are known constants, find c(r,θ ) inside the drop. Do not leave any integrals unevaluated.
3. Use a Laplace transform to solve the wave equation:
2φ
∂x2=1
c2
2φ
∂t2
subject to the boundary condition
φ(0, t) = 0
and to the initial conditions
φ(x, 0) = 0,
∂φ(x, 0)
∂t = 1.
4. The motion of a mass on a spring with damping is governed by
d2x
dt2+ 2αdx
dt + (α2+β2)x=1
mf(t)
where α=c/2m,β=pω2
0α2, and ω2
0=k/m. For unforced motion (f(t) = 0), starting from rest
at x=x0, use LaPlace transforms to determine x(t) for β= 0 and β > 0 (real). For each case, make
a qualitative sketch of xvs. t.
1

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CHE 527 Advanced Applied Mathematical Analysis in Chemical Engineering Fall 2006

Homework 9

Due in class on Tuesday, November 21.

  1. Potential flow past a sphere is governed by

∇^2 φ =

r^2

∂r

r^2 ∂φ ∂r

r^2 sin θ

∂θ

sin θ ∂φ ∂θ

where v = ∇φ = ∂φ ∂r er +

r

∂φ ∂θ eθ is the velocity. Use separation of variables to solve for φ(r, θ) in the domain a ≤ r ≤ ∞ subject to the B.C.’s ∂φ∂r = 0 on r = a, and ∂φ∂r = U∞ cos θ as r → ∞.

  1. Consider the diffusive mass transfer (∇^2 c = 0) of a solute inside a liquid drop subject to a mass transfer boundary condition (−D ∂c∂r = k(c − c 0 ) at r = a). For an axisymmetric case c 0 = c 1 + c 2 cos θ, where c 1 and c 2 are known constants, find c(r, θ) inside the drop. Do not leave any integrals unevaluated.
  2. Use a Laplace transform to solve the wave equation: ∂^2 φ ∂x^2 =

c^2

∂^2 φ ∂t^2 subject to the boundary condition φ(0, t) = 0 and to the initial conditions φ(x, 0) = 0, ∂φ(x, 0) ∂t

  1. The motion of a mass on a spring with damping is governed by d^2 x dt^2 + 2α dx dt + (α^2 + β^2 )x =^1 m f (t)

where α = c/ 2 m, β =

ω 02 − α^2 , and ω^20 = k/m. For unforced motion (f (t) = 0), starting from rest at x = x 0 , use LaPlace transforms to determine x(t) for β = 0 and β > 0 (real). For each case, make a qualitative sketch of x vs. t.