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Main Page Chapter 1 Chapter 2 Chapter 3 Chapter 4 List of Topics
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CHAPTER
4
LAPLACE'S
EQUATION
It
is one of the most important partial differential equations and its solution is
known as potential function or harmonic functions.
in
three dimension
in two
dimension
in
one dimension
In
steady-state case (u is independent
of t) wave and heat equations change
to Laplace's equation.
* So steady-state solution of heat and wave
equation is the solution of Laplace's equation also.
LAPLACES EQUATION IN :
-
Cartesian
coordinates : (x,y,z)
(1)
-
Cylindrical
polar coordinates : (r,q , z)
..(2)
-
Spherical
polar coordinates : (r,q,j)
.(3)

The
upper plate of a parallel-plate capacitor is maintained at 100V, and the lower
plate is maintained at 0V. The plates are 10 cm apart, and they are infinitely
large. Find V in the parallel-plate region.
Let
us set up a coordinate system shown in figure.

So,
the boundary conditions are
V = 0V at y = 0
(1)
and V = 100V at y = 10 cm = 0.1
cm
(2)
\ By symmetry V is a function
of y only and is independent of x and z. Thus, this problem is to solve Laplace equation
i.e.,
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\
..(3)
where A and B are constants.
Applying
(1), V(0) = 0 = B
Applying
(2), V(10) = 0.1 A + B = 100
or, A =
1000
\ From (3) the required charge
V in parallel-plate is
V(y) =
1000y Volt.
Find
the temperature between two parallel plates
x = 0 and x = d
having temperature 0°C and 100°C respectively.
Let
the temperature between two parallel plates be T.

So,
the boundary conditions are
T
= 0° C at
x = 0
and T =
100° C at
x = d
\ T depends only on x and
independent of y and z. Hence Laplace's equation
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becomes ![]()
\ T(x) = Ax + B
So, T(0) = 0 = B and T(d)
= 100 = Ad + B
or, ![]()
\ The required temperature
between the given parallel plates is
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Find
the temperature distribution in the region (i.e. cross-section of a solid
cylinder) whose vertical portion of the boundary is at 20°C , the horizontal portion at 50°C , and the circular portion is insulated (as
in figure).

Let
T be the temperature distribution in
the cross-section area of cylinder. If r
be the radius of the circular area, then
so,
is any point on the
circular boundary.
Since
the circular portion is insulated, heat will not flow along r, so
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\ T depends only on q with boundary condition
T(0) = 50° C and
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Hence
Laplace's equation in polar coordinates becomes
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or,
(1)
\ ![]()
and ![]()
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Hence
from (1) the required temperature-distribution is,
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or, ![]()

Heat
flows from x-axis along circles r = constant (dashes in figure) to the y-axis.
The
inner and outer radii of two concentric, thin conducting spherical shells are a
and b respectively. The space between the shells is filled with an insulating
material. The inner shell is maintained at a potential V1 and the
outer at a potential V2 (as figure). Determine the potential
distribution in the insulating material by solving Laplace's equation in
spherical polar coordinates.

Laplace's
equation in spherical coordinates is

For
a given fixed electric potential distribution
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of
a sphere of radius R, always
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i.e. u is independent of q.
The
boundary conditions are
..(2)
Now,
for symmetry
equation (1) becomes
(3)
Again, ![]()
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