tute sheet_sepration of var
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Tutorial sheet -5
Q1. Solve the following first order partial differential equations by separating
the variables:
(a) 0=∂
∂−
∂
∂
y
u x
x
u
(b) 02 =∂
∂−
∂
∂
y
u y
y
u x
Q2. A semi-infinite rectangular metal plate occupies the region ∞≤≤ x0 andb y ≤≤0 in the x-y plane. The temperature at the far end of the plate and along
its two long sides is fixed at 0°C. If the temperature of the plate at x=0 is alsofixed and is given by )( y f , fine the steady state temperature distribution
),( y xu of the plate. Hence find the temperature distribution if 0)( u y f = , where
0u is a constant.
Q3. Obtain a separable solution describing a particle confined to a box of side a
(ψ must vanish at the walls of the box). Show that the energy of the particle can
only take the quantized values
)(2
222
2
22
z y x nnnma
E ++=π , where x
n , yn and z n are integers.
Q4.The wave equation describing the transverse vibrations of a stretched
membrane under tension ‘T’ and having a uniform surface density ρ is
2
2
2
2
2
2
)(t
u
y
u
x
uT
∂
∂=
∂
∂+
∂
∂ ρ
Find a separable solution appropriate to a membrane stretched on a frame of
length ‘a’ and width ‘b’, showing that the natural angular frequencies of such a
membrane are given by
)(2
2
2
222
b
m
a
nT +=
ρ
π ω ,
Where ‘n’ and ‘m’ are any positive integers
Q5. Denoting the three terms of 2∇ in spherical polars by 2
r ∇ ,2θ ∇ ,
2
φ ∇ in an
obvious way, evaluate ur 2
∇ , etc. For the two functions given below and verify
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that, in each case, although the individual terms are not necessarily zero their
sum 2∇ u is zero. Identify the corresponding values of l and m.
(a)
2
1cos3)(),,(
2
3
2 −+=
θ φ θ
r
B Ar r u
(b) θ θ φ θ ir
B Ar r u expsin)(),,(
2+=
Q6. A circular disc of radius ‘a’ is heated in such a way that its perimeter a= ρ
has a steady temperature distribution φ 2cos B A+ , where ρ and are plane
polar coordinates, A and B are constants. Find the temperature ),( φ ρ T
everywhere in the region a< ρ .
Q7. Prove that the potential for a< ρ associated with a vertical split cylinder of radius ‘a’, the two halves of which 0(cos >φ and )0cos <φ are maintained at
equal and opposite potentials ±V, is given by
φ ρ
π φ ρ )12cos()(
12
)1(4),(
12
0 ++
−∑=
+∞
=n
an
V u
n
n
n
Q8. Two identical copper bars each of length ‘a’. Initially one is at C ο
0 and the
other at C ο 100 ; they are then joined together end to end and thermally isolated.
Obtain in the form of a Fourier series an expression ),( t xu for the temperatureat any point a distance x from the join at a later time‘t’. Bear in mind the heat
flow conditions at the free ends of the bar.
Taking a=0.5m estimate the time it takes for one of the free ends to attain a
temperature of C ο
55 . The thermal conductivity of copper is 3.8x102Jm-1K -1s-1,
and its specific heat capacity is 3.4x106Jm-3K -1.