11
Engineering in EEE 303: Signals and Linear Systems The Fourier Transform Let be a nonperiodic signal of finite duration, i.e., Let us form a periodic signal by extending to as, , [i.e., the period is infinity] Then, (01) Or, Let us now define as, Thus, . Substituting this in equation (01) we get, As , . Let us assume . Thus, Or, (02)

Signals and Systems 05

Embed Size (px)

DESCRIPTION

Engineering in EEE 303: Signals and Linear SystemsThe Fourier TransformFourier Spectra

Citation preview

Engineering in EEE 303: Signals and Linear Systems

The Fourier Transform

Let be a nonperiodic signal of finite duration, i.e.,

Let us form a periodic signal by extending to as,

,

[i.e., the period is infinity]

Then,

(01)Or,

Let us now define as,

Thus,

.

Substituting this in equation (01) we get,

As , . Let us assume.

Thus,

Or,

(02)

in equation (02) is called the Fourier Integral. Thus a finite duration signal is represented by Fourier integral instead of Fourier series.

The function is called the Fourier transform of.

Symbolically these two pairs are represented as,

And

Alternatively,

.Fourier Spectra

The Fourier transform is, in general, complex, and it can be expressed as,

If is real,

Thus,

Therefore, we can conclude that for real signal, the amplitude spectrum is an even function and the phase spectrum is an odd function of .

The condition for the convergence of Fourier transform is the same as the Fourier series.

Example1. Find the Fourier transform of

.2. Find the Fourier transform of .

3. Find the inverse Fourier transform of .

.

Thus, or,

.

4. Find the inverse Fourier transform of .

Thus,

We know, ; Thus,

5. Find the Fourier transform of the rectangular pulse shown in Figure.

The magnitude spectrum is, , and the phase spectrum is, .6. Find the inverse Fourier transform of the rectangular spectrum shown below.

. The plot is shown in Figure above.Some Properties of Fourier Transform

1. Symmetry property: If . (duality property)

Example: Apply symmetry property to show that .

2. Scaling Property: If .

3. Time-shifting Property: If .4. Frequency-shifting Property: If .

Example: Find the Fourier transform of the gate pulse shown in Figure below.

We get the Fourier transform by applying time-delay property to the F.T. of rectangular pulse (symmetrical).

Thus,

.

Example: Sketch the Fourier transform of using frequency shifting property. [property 4] . Therefore, . The sketch is shown in Figure below. Here, .

5. Time and Frequency convolution: .

6. Time differentiation and time integration: .

(a)

Therefore, =,

or, . (b)

Using convolution property,

Therefore, .Example: Using the time-differentiation property, find the F.T. of the triangle illustrated in figure below.

Performing F.T. of the first equation,

EMBED Equation.DSMT4

Fourier transform of periodic signalLet,

(periodic). Performing L.T. we get,

.Therefore, the Fourier transform of a periodic signal is a train of impulses occurring at harmonically related frequencies where the impulse strength is, .For example, consider the Fourier series and Fourier transform of the signal. Energy of aperiodic signal

Energy of aperiodic signal,

Or,

i.e., . This relation is called the Parsivals relation for aperiodic signal.

The term is called the energy spectral density of the signal. If it is integrated over all the frequencies and multiplied by we get the energy of the aperiodic signal.

Example: The signals shown in Figure below are modulated signal with carrier. Find the Fourier transform of these signals.

(a) Here a triangular pulse of width is modulated with a carrier . Now the Fourier transform of triangular pulse is, .

And the F.T. of carrier is,

Therefore,

Or,

[ans]

(b) This is the time-shifted version of (a). Here the time-shift is . Time shift corresponds to phase shift of in frequency domain.The result is, .(c) Here cosine wave is multiplied by a rectangular pulse of width with a time-shift of .

Here the F.T. of rectangular pulse is (symmetric w.r.t. y-axis), . is the same as in (a). Thus,

EMBED Equation.DSMT4 Hence, . [ans]Signal transmission through LTI systemWe know, . Using convolution property, .Therefore, .

Remember that, is called the frequency response of a system. In order to find the response of a system using F.T. we have to get first. Then we will get using inverse Fourier transform of . Example

Find the response of a system shown below when an input of the system is.

Performing F.T. on both side,

. But,

Performing inverse Fourier transform, [ans]If , then the characteristic mode of input and output are the same and resonance will occur. If we put the condition in , it will become indeterminate. We can find using LHospital rule.Hence,

.System response to periodic inputLet, . Performing F.T. we get, .Now, .

Performing inverse F.T. we get,

Therefore, the output will be also periodic. The amplitude of the nth harmonic components will be, .

Some More Examples1. Determine the Fourier transform of the complex sinusoidal pulse, .The function z(t) may be expressed as, where, .

In Fourier transformed domain, . [frequency shifting property]

Now, . Here . Thus, .Hence,

[Ans]

2. Show that the differentiation in frequency corresponds to multiplication in time by -jt.

Therefore,

Hence the statement.

3. Use the frequency differentiation property to find the F.T. of .

We know,

Therefore,

Or, ; or, [Ans]4. Let the input to a system with impulse response be . Find the output of the system .

. Now and .

. Performing inverse Fourier transform,

[Ans]Windowing operationThe process of truncating a function is called windowing. It is represented mathematically by multiplying the signal, by a window function, . If is the windowed signal, .In frequency domain it can be viewed as, . The windowing operation and its effect in frequency domain is shown in figure below.

The general effect of window is to smooth detail in and introduce oscillation near discontinuities in. The smoothing is the consequence of the main lobe of width (for rectangular window) while the oscillations are due to the oscillations in the side lobes of .Fourier Transform of

1. ; We know that, and

Thus, .

[Ans]

2.

Therefore,

EMBED Equation.DSMT4

[Ans]Example

The output of a system in response to an input is. Find the frequency response and the impulse response of the system.

,

EMBED Equation.DSMT4 .

EMBED Equation.DSMT4

Performing inverse F.T. we get, .

[Ans]

Find the frequency response and the impulse response of the system .Signal distortion during transmission

For distortionless transmission through an LTI system we require that the exact input signal shape be reproduced at the output although its amplitude may be different and it may be delayed in time. Therefore,

.Thus for distortionless transmission the system must have, .

and .

i.e., the amplitude of must be constant over the entire frequency range and the phase of must be linear with frequency.

A system may have flat amplitude response, but it will be distorted if system is not constant.Application of Fourier transform

1. Modulation and demodulation

To allow different frequency band for different channel

For effective radiation of signal antenna size must be of the order of the wavelength of the signal to be radiated. Shifting the signal to the higher frequency by modulation solves the problem.

Figure left shows the process of amplitude modulation with a sinusoidal carrier. We choose for convenience.

The original signal can be recovered by modulating with the same sinusoidal carrier and applying low-pass filter to the result.

Or,

EMBED Equation.DSMT4 If modulator and demodulator are not synchronized,

EMBED Equation.DSMT4 .In this case, , the output will be zero. For maximum output signal the oscillators must be in phase. This requires careful synchronization between modulator and demodulator._1262103233.unknown

_1262118523.unknown

_1262599263.unknown

_1262601626.unknown

_1263230879.unknown

_1263237795.unknown

_1263240858.unknown

_1263241612.unknown

_1263241778.unknown

_1263242192.unknown

_1263242305.unknown

_1263242367.unknown

_1263241796.unknown

_1263241676.unknown

_1263241072.unknown

_1263241493.unknown

_1263240966.unknown

_1263238197.unknown

_1263238307.unknown

_1263238603.unknown

_1263238240.unknown

_1263237968.unknown

_1263237992.unknown

_1263237874.unknown

_1263236097.unknown

_1263236346.unknown

_1263236441.unknown

_1263236665.unknown

_1263236372.unknown

_1263236264.unknown

_1263236294.unknown

_1263236252.unknown

_1263231319.unknown

_1263231501.unknown

_1263236069.unknown

_1263231390.unknown

_1263231209.unknown

_1263231260.unknown

_1263231096.unknown

_1262602864.unknown

_1262603411.unknown

_1262603602.unknown

_1263230587.unknown

_1262603510.unknown

_1262602973.unknown

_1262603318.unknown

_1262602895.unknown

_1262601827.unknown

_1262602811.unknown

_1262602826.unknown

_1262601916.unknown

_1262601704.unknown

_1262601735.unknown

_1262601637.unknown

_1262601070.unknown

_1262601491.unknown

_1262601556.unknown

_1262601597.unknown

_1262601523.unknown

_1262601308.unknown

_1262601368.unknown

_1262601144.unknown

_1262599520.unknown

_1262600861.unknown

_1262601011.unknown

_1262600808.unknown

_1262599433.unknown

_1262599459.unknown

_1262599387.unknown

_1262596703.unknown

_1262598118.unknown

_1262598579.unknown

_1262599067.unknown

_1262599182.unknown

_1262598961.unknown

_1262598342.unknown

_1262598455.unknown

_1262598194.unknown

_1262597171.unknown

_1262597469.unknown

_1262597622.unknown

_1262597405.unknown

_1262596901.unknown

_1262597100.unknown

_1262596761.unknown

_1262596005.unknown

_1262596286.unknown

_1262596506.unknown

_1262596617.unknown

_1262596457.unknown

_1262596163.unknown

_1262596187.unknown

_1262596134.unknown

_1262119073.unknown

_1262119110.unknown

_1262119176.unknown

_1262119077.unknown

_1262118854.unknown

_1262118906.unknown

_1262118561.unknown

_1262107719.unknown

_1262117767.unknown

_1262118123.unknown

_1262118384.unknown

_1262118439.unknown

_1262118224.unknown

_1262117903.unknown

_1262118088.unknown

_1262117850.unknown

_1262115765.unknown

_1262116066.unknown

_1262117111.unknown

_1262108773.unknown

_1262108814.unknown

_1262108911.unknown

_1262107996.unknown

_1262107859.unknown

_1262105506.unknown

_1262106980.unknown

_1262107482.unknown

_1262107680.unknown

_1262107089.unknown

_1262106659.unknown

_1262106795.unknown

_1262106127.unknown

_1262104603.unknown

_1262105029.unknown

_1262105113.unknown

_1262104728.unknown

_1262103740.unknown

_1262103795.unknown

_1262103620.unknown

_1261597875.unknown

_1261934979.unknown

_1261945382.unknown

_1262102492.unknown

_1262103136.unknown

_1262103205.unknown

_1262103092.unknown

_1261945870.unknown

_1261946151.unknown

_1261945463.unknown

_1261945787.unknown

_1261943911.unknown

_1261944204.unknown

_1261944434.unknown

_1261943987.unknown

_1261935549.unknown

_1261943519.unknown

_1261935130.unknown

_1261599654.unknown

_1261600052.unknown

_1261933766.unknown

_1261934461.unknown

_1261933542.unknown

_1261599787.unknown

_1261599952.unknown

_1261599693.unknown

_1261599312.unknown

_1261599433.unknown

_1261599488.unknown

_1261599417.unknown

_1261599141.unknown

_1261599212.unknown

_1261599089.unknown

_1261595571.unknown

_1261596819.unknown

_1261597356.unknown

_1261597432.unknown

_1261597667.unknown

_1261597410.unknown

_1261596956.unknown

_1261597268.unknown

_1261596871.unknown

_1261596393.unknown

_1261596568.unknown

_1261596678.unknown

_1261596462.unknown

_1261596124.unknown

_1261596157.unknown

_1261595989.unknown

_1261588796.unknown

_1261590232.unknown

_1261590324.unknown

_1261595461.unknown

_1261590270.unknown

_1261588896.unknown

_1261590152.unknown

_1261588852.unknown

_1261588097.unknown

_1261588644.unknown

_1261588711.unknown

_1261588366.unknown

_1261587943.unknown

_1261588061.unknown

_1261587810.unknown