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Review of Partial Differential Equations

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Review of Partial Differential Equations

We are used to the function of a single variable, say


f = f(x), “function” meaning that for any given
value of x, there exists one and only one value of f.
And we know that

df f  x Δx − f  x 
= f '  x =lim ………… (1)
dx Δx 0 Δx

which is the first derivative of the function. We


d2 f
denote the second derivative as 2
. There are, of
dx
course, higher derivatives.

We also know about the chain rule. If say we have


g(f) where f = f(x), then

dg dg df
g '  x = = ⋅ ……………………….. (2)
dx df dx

The chain can of course be longer than that above.

Whenever we have a function of two independent


variables, say f = f(x,y), “independent” meaning x is
not a function of y nor vice versa, then
∂f ∂f
df = dx dy ………………………… (3)
∂x ∂y

∂f f  x Δx , y − f  x , y 
where =lim ……… (4)
∂ x Δx  0 Δx
is the “partial derivative of f with respect to x”, that
is, the derivative of f while keeping y at some
∂f
constant value; similarly, is the partial
∂y
derivative of f with respect to y. We can of course
extend this to functions of more than two
independent variables.
We can manipulate Eq. (3) in the following manner:
df ∂ f ∂ f dy df ∂ f dx ∂ f
=  or =  …… (5)
dx ∂ x ∂ y dx dy ∂ x dy ∂ y
We have a chain rule for partial derivatives. If
f = f(u,v) and u = u(x,y) and v = v(x,y), then:
∂ f ∂ f ∂u ∂ f ∂v ∂ f ∂ f ∂u ∂ f ∂ v
= ⋅  and =  ⋅ … (6)
∂ x ∂u ∂ x ∂v ∂ x ∂ y ∂u ∂ y ∂v ∂ y
which chain is again extendable to three or more,
and the functions can be of three or more variables.
If we have the special case, f = f(x,y) where x = x(t) and
y = y(t), then
df ∂ f dx ∂ f dy
=  …………………………… (7)
dt ∂ x dt ∂ y dt
This form is called the parametric representation of
the function f, where t is the “parameter” and x and
y are the “coordinates”.
Unlike total differentials, partial differentials, e.g.
∂ f or ∂ x , have no meaning by themselves, nor are
they operable like fractions.
The higher order partial derivatives may be
described in the following manner:

2
∂ f
=
∂  
∂f
∂x ; 2
∂ f
=
∂f

∂y  
∂x
2
∂x ∂x∂ y ∂x
Examples of partial differential equations:
2
∂u ∂u
=c 2⋅ 2 (One-dimensional heat equation)
∂t ∂x
2 2
∂u ∂u
2
 2 (Two-dimensional Laplace equation)
∂x ∂ y
For subsequent applications, we can now consider the
∂ ∂ ∂
operator ∇ =   , shortened verbally
∂x ∂ y ∂z
as “del”, which has no meaning by itself but is used
merely to shorten writing of long equations.
Thus, if we take the Laplacian (del-squared) of u in
2 2 2
∂u ∂u ∂u
three dimensions, then ∇ u= 2  2  2 is
2

∂x ∂ y ∂z
the Three-dimensional Laplace equation.

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