Digital Signal Processing Reference
In-Depth Information
20.3.2 Functions of real and imaginary parts
Let z = x + jy so that x and y denote the real and imaginary parts of z .Let
f ( x, y ) denote the function g ( z, z ) regarded as a function of the two real vari-
ables x and y . Thus the original function h ( z ) now has three different notations: 1
h ( z )= g ( z, z )= f ( x, y ) .
(20 . 22)
Now, how are the partial derivatives ∂f ( x, y ) /∂x and ∂f ( x, y ) /∂y related to the
partial derivatives ∂g ( z, z ) /∂z and ∂g ( z, z ) /∂z ?
The answer is (see proof
below):
=0 . 5 ∂f ( x, y )
and
=0 . 5 ∂f ( x, y )
∂x
.
(20 . 23)
∂g ( z, z )
∂z
j ∂f ( x, y )
∂y
∂g ( z, z )
∂z
+ j ∂f ( x, y )
∂y
∂x
By adding and subtracting these two equations we obtain
.
(20 . 24)
The distinction between the notations h, g ,and f is usually clear from the con-
text, and we often simplify by saying ∂g/∂x = ∂g/∂z + ∂g/∂z , and so forth.
The relation (20.23) is often summarized in operator form as shown below:
= ∂g ( z, z )
∂z
and
= j ∂g ( z, z )
∂z
∂f ( x, y )
∂x
+ ∂g ( z, z )
∂z
∂f ( x, y )
∂y
∂g ( z, z )
∂z
∂z =0 . 5
and
=0 . 5
.
∂y
∂z
∂y
∂x
j
∂x + j
(20 . 25)
Proof of Eq. (20.23). From g ( z, z )= f ( x, y ) we see that
∂g
∂z = ∂f
∂x
∂z + ∂f
∂y
∂z
∂g
∂z
= ∂f
∂x
∂x
∂z
+ ∂f
∂y
∂y
∂z
and
∂x
∂y
Substituting
∂x
∂z
∂x
∂z
∂y
∂z =
∂y
∂z
=0 . 5 ,
=0 . 5 ,
0 . 5 j,
=0 . 5 j,
(which follows from x =( z + z ) / 2and y =( z −z ) / 2 j ) we therefore obtain
∂z =0 . 5 ∂f
=0 . 5 ∂f
∂g
∂x − j ∂f
∂g
∂z
∂x + j ∂f
and
∂y
∂y
This proves Eq. (20.23).
1 Given h ( z ), we can substitute z = x + jy and obtain the form h ( z )= f ( x, y ) . In this
expression if we substitute x =( z + z ) / 2and y =( z − z ) / 2 j , then we get the form h ( z )=
g ( z, z ).
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