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SIGNALS AND THEIR REPRESENTATION

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Title: SIGNALS AND THEIR REPRESENTATION


1
  • SIGNALS AND THEIR REPRESENTATION
  • Signals can be of two types
  • Continuous
  • (ii) Discrete
  • Most of the signals are inherently

2
  • continuous but for use in computer they are
    discretised or sampled at regular intervals.
  • Thus a voltage can be recorded continuously
    with the help of a pen-recorder but if we want
    to use

3
  • it for some computational purpose, we have to
    discretise it in magnitude as well as in time
    (Fig. 2.9 a, b).

4
f (nT)
f (t)
0
0
t
T
2T
nT
t
Fig. 2.9(b)
Fig. 2.9(a)
5
  • The values sampled at regular intervals give some
    idea about the nature of variation of the
    original function f (t) with t. However, if the
    sampling interval is increased, then

6
  • many important informations about the signal will
    be lost.
  • So for getting all the important information
    about the original continuous signal, it is
    desirable that

7
  • the sampling time is made very very small such
    that no peak or trough is missed out between two
    successive samples.
  • This necessitates that we sample

8
  • the signal at a rate to trap a maximum or a
    minimum. This is ensured if the sampling
    frequency f s ? 2 fmax ,where fmax is the highest
    frequency present in the signal.

9
  • UNIT STEP
  • When we switch on a constant voltage source to
    excite a circuit, the applied voltage is zero
    before the switching instant and remains constant
    after that (Fig. 2.10).

10
t 0
R
V (t)

Vc
-
Vc
V (t)
L
t
0
Fig. 2.10
11
  • If the magnitude of the voltage is unity (or
    normalised to some scale to unity), it is called
    a unit step.
  • Mathematically we write this as
  • u (t) 1 t ? 0
  • 0 otherwise

12
  • UNIT RAMP
  • If a function increases continuously at a
    uniform rate, it is called a ramp function.
  • r (t) k t t ? 0
  • 0 otherwise
  • When k 1, it is called a unit ramp.

13
  • UNIT IMPULSE
  • When we apply a very large force for a very short
    duration such that neither the magnitude of the
    force nor the duration is measurable,

14
  • but their product is finite and measurable, it is
    an impulse. If the product is unity, it is a unit
    impulse.

15
The product of f (t) and ?t is the area of the
thin rectangular strip. (Fig 2.11).
?


f (t)
t
? t
Fig. 2.11
16
  • We denote this function as ?(t) which is defined
    mathematically as
  • Ideally ? (t) 0 at t 0 to ?
  • and t 0- to - ?
  • 1 at t 0

17
  • An approximation to this is a situation when a
    cricket ball is hit by a bat the time of
    contact is very small, and the force applied is
    very large, but the change in momentum is finite.

18
  • Signals can also be classified a deterministic
    or random. At this moment, we shall not
    consider random signals, and our studies will be
    restricted to deterministic signals.

19
  • A shifted signal f(t ?) is obtained when f(t)
    is shifted to the right by an interval ? in time.
    Mathematically this will be written as (Fig.
    2.12)
  • f1 (t) f (t - ?) u (t - ?).

20

f1 (t- ? )
f1 (t)
f (t)
0
t
t
?
Fig.2.12(a)
Fig.2.12(b)
21
  • This is multiplied by u (t - ?) to indicate that
    the function f (t) does not exist before t 0,
    and in electrical engg. we deal with such
    functions most of the time. Before switching a
    voltage at t 0, the circuit does not receive
    any excitation.

22
  • Thus an exponentially decaying voltage or
    current function, say 5e-3t, will be as shown
    by the solid curve and strictly speaking should
    be written as 5e-3t u(t) (see Fig. 2.13).

23

Fig. 2.13
The function 5e-3t extends to the negative
region as shown by the dotted portion, upto - ?.
24
  • We can express any function mathematically by the
    sum of the above regular functions (defined upto
    t ?).
  • For example, a rectangular function shown in
    Fig. 2.14 is given by (Fig 2.14)

25
10
Fig. 2.14
3
t
3
10
f2 (t)
t

f1(t)
-10
t
26
  • f(t) 10, 0 ? t ? 3
  • 0 otherwise
  • f1 (t) f2(t)
  • 10 u (t) 10 u (t-3)

27
  • Example
  • Express a train of rectangular pulses in terms of
    regular functions.

V0
0
T1
T2
T1 T2
2T2
T1 2T2
t
28
  • The first pulse can be written as
  • f1 (t) V0 u(t) u (t T1)
  • The Second Pulse can be written as a shifted
    f1(t)
  • as f2 (t) f1(t T2) u (t T2).
  • similarly, f3 (t) f1(t-2T2) u (t-2T2)
  • .. and so on.

29
  • Thus
  • f (t) f1(t) f2(t) f3(t) .?
  • V0 u (t) u (t-T1)
  • u (t T2) (t T1-T2)
  • u (t 2T2) u (t T1 2T2) . ?

30
  • Exercise
  • Express the following functions mathematically
    in terms of regular continuous functions.
    (Fig.2.16)

31
f (t)

f (t)
10
k
0
4
8
t
0
T
t
Fig 2.16 (ii)
f (t)
Fig 2.16 (i)
2
16
0
8
Fig 2.16 (iii)
32
f (t)
10 sin 6 ? t
Fig 2. 16 (iv)
t
0
T
10
Fig 2.16 (v)
f (t)
0
3
4
t
1
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