24 C H A P T E R 0: From the Ground Up!
The relation between the complex exponentials and the sinusoidal functions is of great importance
in signals and systems analysis. Using Euler’s identity the cosine can be expressed as
cos(θ)=Re[ejθ]=
ejθ+e−jθ
2
(0.19)
while the sine is given by
sin(θ)=Im[ejθ]=
ejθ−e−jθ
2 j
(0.20)
Indeed, we have
ejθ=cos(θ)+jsin(θ)
e−jθ=cos(θ)−jsin(θ)
Adding them we get the above expression for the cosine, and subtracting the second from the first we
get the given expression for the sine. The variableθis in radians, or in the corresponding angle in
degrees (recall that 2πradians equals 360 degrees).
These relations can be used to define the hyperbolic sinusoids as
cos(jα)=
e−α+eα
2
=cosh(α) (0.21)
jsin(jα)=
e−α−eα
2
=−sinh(α) (0.22)
from which the other hyperbolic functions are defined. Also, we obtain the following expression for
the real-valued exponential:
e−α=cosh(α)−sinh(α) (0.23)
Euler’s identity can also be used to find different trigonometric identities. For instance,
cos^2 (θ)=
[
ejθ+e−jθ
2
] 2
=
1
4
[2+ej^2 θ+e−j^2 θ]=
1
2
+
1
2
cos( 2 θ)
sin^2 (θ)= 1 −cos^2 (θ)=
1
2
−
1
2
cos( 2 θ)
sin(θ)cos(θ)=
ejθ−e−jθ
2 j
ejθ+e−jθ
2
=
ej^2 θ−e−j^2 θ
4 j
=
1
2
sin( 2 θ)
0.4.3 Phasors and Sinusoidal Steady State
A sinusoidx(t)is a periodic signal represented by
x(t)=Acos( 0 t+ψ) −∞<t<∞ (0.24)
whereAis the amplitude, 0 = 2 πf 0 is the frequency in rad/sec, andψis the phase in radians. The
signalx(t)is defined for all values oft, and it repeats periodically with a periodT 0 = 1 /f 0 (sec), so