The most ubiquitous and important signal in electrical
engineering is the sinusoid.
st=Acos2πft+φ
or
Acosωt+φ
s
t
A
2
f
t
φ
or
A
ω
t
φ
(1)
AA is known as the sinusoid's
amplitude, and determines the sinusoid's size.
The amplitude conveys the sinusoid's physical units (volts,
lumens, etc). The
frequency
ff has units of Hz (Hertz) or
s-1
s
, and determines how rapidly the sinusoid oscillates
per unit time. The temporal variable
t
t always has units of seconds, and thus the frequency
determines how many oscillations/second the sinusoid has. AM
radio stations have carrier frequencies of about 1 MHz (one
mega-hertz or
106
10
6
Hz), while FM stations have carrier frequencies of
about 100 MHz. Frequency can also be expressed by the symbol
ωω, which has units of
radians/second. Clearly,
ω=2πf
ω
2
f
. In communications, we most often express frequency in
Hertz. Finally,
φφ
is the
phase, and determines the sine wave's behavior
at the origin (
t=0
t
0
). It has units of radians, but we can express it in
degrees, realizing that in computations we must convert from
degrees to radians. Note that if
φ=-π2
φ
2
, the sinusoid corresponds to a sine function, having a
zero value at the origin.
Asin2πft+φ=Acos2πft+φ-π2
A
2
f
t
φ
A
2
f
t
φ
2
(2)
Thus, the only difference between a sine and cosine signal is
the phase; we term either a sinusoid.
We can also define a discrete-time variant of the sinusoid:
Acos2πfn+φ
A
2
f
n
φ
. Here, the independent variable is
nn and represents the
integers. Frequency now has no dimensions, and takes on values
between 0 and 1.
Show that
cos2πfn=cos2πf+1n
2
f
n
2
f
1
n
, which means that a sinusoid having a frequency
larger than one corresponds to a sinusoid having a frequency
less than one.
As
cosα+β=cosαcosβ-sinαsinβ
α
β
α
β
α
β
,
cos2πf+1n=cos2πfncos2πn-sin2πfnsin2πn=cos2πfn
2
f
1
n
2
f
n
2
n
2
f
n
2
n
2
f
n
.
Notice that we shall call either sinusoid an analog
signal. Only when the discrete-time signal takes on a finite
set of values can it be considered a digital signal.
Can you think of a simple signal that has a finite number
of values but is defined in continuous time? Such a signal
is also an analog signal.
A square wave takes on the values
1
1
and
-1
-1
alternately. See the plot in the module Elemental Signals.
The basic idea of communication engineering is to use a
signal's parameters to represent either real numbers or other
signals. The technical term is to modulate the
carrier signal's parameters to transmit
information from one place to another. To explore the notion
of modulation, we can send a real number (today's temperature,
for example) by changing a sinusoid's amplitude accordingly.
If we wanted to send the daily temperature, we would keep the
frequency constant (so the receiver would know what to expect)
and change the amplitude at midnight.
We could relate temperature to amplitude by the formula
A=A01+kT
A
A0
1
k
T
, where
A0
A0 and
kk are
constants that the transmitter and receiver must
both know.
If we had two numbers we wanted to send at the same time, we
could modulate the sinusoid's frequency as well as its
amplitude. This modulation scheme assumes we can estimate the
sinusoid's amplitude and frequency; we shall learn that this is
indeed possible.
Now suppose we have a sequence of parameters to send. We have
exploited all of the sinusoid's two parameters. What we can
do is modulate them for a limited time (say
TT seconds), and send two
parameters every TT. This simple
notion corresponds to how a modem works. Here, typed
characters are encoded into eight bits, and the individual
bits are encoded into a sinusoid's amplitude and frequency.
We'll learn how this is done in subsequent modules, and more
importantly, we'll learn what the limits are on such digital
communication schemes.
"Electrical Engineering Digital Processing Systems in Braille."