Fourier Transform of Basic Signals - 4.4 | Module 4 - Fourier Transform Analysis of Continuous-Time Aperiodic Signals | Signals and Systems
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4.4 - Fourier Transform of Basic Signals

Practice

Interactive Audio Lesson

Listen to a student-teacher conversation explaining the topic in a relatable way.

Rectangular Pulse Transform

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0:00
Teacher
Teacher

Today we're going to explore the Fourier Transform of the rectangular pulse. Can anyone remind me what a rectangular pulse looks like?

Student 1
Student 1

Isn't it a signal that stays at 1 for a time period, like T seconds, and is 0 outside that range?

Teacher
Teacher

Exactly! We denote it as `rect(t/T)`. Now, when we derive its Fourier Transform, we find it results in: X(jω) = T * sinc(ωT/(2π)). Can someone explain what the sinc function represents here?

Student 2
Student 2

The sinc function relates to the spread of frequencies! A wider pulse means a narrower bandwidth in frequency.

Teacher
Teacher

Right! The key takeaway is the inverse relationship between time duration and bandwidth. A wider pulse compresses its frequency range. Remember: T and bandwidth are inversely related, something I like to call the 'T-Bandwidth Law'.

Student 3
Student 3

So, if I increase T, I will see a narrower main lobe in the frequency domain?

Teacher
Teacher

Yes, that's correct! Great connection. Now let's summarize: the rectangular pulse Fourier Transform results in a sinc function indicating the relationship between time domain width and frequency.

Unit Impulse Function

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0:00
Teacher
Teacher

Next, let's discuss the unit impulse function, delta(t). Who can describe its key characteristic?

Student 4
Student 4

It's an ideal signal with infinite amplitude at t=0 and zero elsewhere, right?

Teacher
Teacher

Exactly! When we derive its Fourier Transform, we find X(jω) = 1. What does this indicate about the impulse function's frequency content?

Student 1
Student 1

It means it contains all frequencies equally, since it's constant across all frequencies!

Teacher
Teacher

Yes! This is a key feature of the impulse functionβ€”it represents every frequency component at equal amplitude. A good way to remember it is that impulse functions are the 'musical note that plays them all at once'.

Student 3
Student 3

So, anything applied at a single point in time captures all possible frequencies?

Teacher
Teacher

Yes! Great understanding. In summary, the unit impulse function's Fourier Transform is constant across all frequencies, showing its broad frequency representation.

Unit Step Function Transform

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0:00
Teacher
Teacher

Now, let's move on to the unit step function, u(t). What do we know about its definition?

Student 4
Student 4

It's zero for t < 0 and one for t >= 0.

Teacher
Teacher

Correct! However, since it's not absolutely integrable, deriving its Fourier Transform can be tricky. One way to think of it is through its relationship with the delta function. Can anyone explain how?

Student 2
Student 2

We can use differentiation! Because the derivative of u(t) is delta(t), we can apply the differentiation property of the Fourier Transform.

Teacher
Teacher

Exactly! We find that F{u(t)} = 1/(jω) + π*delta(ω). The first term represents the frequency content from the step change, while the delta term accounts for the DC component. Let's remember: 'Steps lead to ans w/ a delta.' Can someone elaborate on how this relates to frequency?

Student 1
Student 1

The step function emphasizes the lower frequencies, while the delta term adds a DC offset!

Teacher
Teacher

Great job, everyone! So to summarize: the unit step function has a Fourier Transform of X(jω) = (1/(jω)) + π*delta(ω), highlighting its unique frequency attributes.

Exponential Signal Transform

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0:00
Teacher
Teacher

Now, let's discuss the exponential signals. We start with the real decaying exponential, x(t) = e^(-at)u(t). What's the Fourier Transform we derive here?

Student 3
Student 3

That would be X(jω) = 1/(a + jω) after solving the integral.

Teacher
Teacher

Correct! Here, we see the characteristics of a decaying exponential—its spectrum is highest at ω=0 and rolls off with increasing frequencies. How about the complex exponential, e^(jω₀t)?

Student 4
Student 4

For that, the Fourier Transform results in X(jω) = 2π*delta(ω - ω₀). It has an impulse at the specific frequency!

Teacher
Teacher

That's right! The complex exponential captures a single frequency component, demonstrating how it maps to an impulse in the frequency domain. Remember: 'Complex e measures just one note, represented by an impulse in frequency.'

Student 2
Student 2

So, these exponential signals reveal how frequency and time domain properties are linked!

Teacher
Teacher

Absolutely! As we summarize: the Fourier Transform of real and complex exponentials shows their critical frequency characteristics and retains the essence of frequency-time relationships.

Introduction & Overview

Read a summary of the section's main ideas. Choose from Basic, Medium, or Detailed.

Quick Overview

This section covers the Fourier Transforms of fundamental signals including rectangular pulse, unit impulse function, unit step function, and exponential signals.

Standard

The section explores the Fourier Transforms of key basic signals, detailing their time domain definitions, derivations, results, and interpretations. It highlights the significance of understanding these transforms as foundational blocks for signal analysis.

Detailed

Fourier Transform of Basic Signals

Understanding the Fourier Transforms of fundamental signals is essential as they serve as building blocks and canonical examples for broader signal analysis. This section covers various common waveforms and their Fourier Transforms:

Key Transformations:

  • Rectangular Pulse (rect(t/T)): Defined as having a constant amplitude of 1 for a duration of T seconds centered at t=0, the Fourier Transform results in a sinc function that illustrates the inverse relationship between time duration and bandwidth.
  • Unit Impulse Function (delta(t)): An idealized signal capturing all frequency components equally, resulting in a constant value of 1 across all frequencies in the Fourier Transform.
  • Unit Step Function (u(t)): Defined as 0 for t < 0 and 1 for t >= 0, the Fourier Transform can be described as a combination of terms that represents both its frequency content and DC component.
  • Exponential Signals: Both decaying exponentials and complex exponentials are addressed, with clear derivations showing that their Fourier Transforms reveal their frequency characteristics effectively.

The section emphasizes how the Fourier Transforms of these basic signals help provide insights into the frequency content of more complex signals.

Audio Book

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Rectangular Pulse

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4.4.1 Rectangular Pulse (rect(t/T))

Time Domain Definition:

The rectangular pulse, denoted as rect(t/T) or Ξ (t/T), is a signal that has a constant amplitude of 1 for a duration of T seconds, centered at t=0, and is 0 everywhere else.

x(t) = 1, for |t| <= T/2
x(t) = 0, for |t| > T/2

Derivation of FT:

X(j*omega) = Integral from t = -T/2 to t = +T/2 of (1 * e^(-j * omega * t) dt)
Solving this integral involves direct integration of the complex exponential.

Fourier Transform Result:

X(jomega) = T * sinc(omega * T / (2pi))
(Note: The sinc function is defined as sinc(x) = sin(pix) / (pix). Sometimes the unnormalized sinc, Sa(x) = sin(x)/x, is used, in which case the argument would be omega*T/2).

Interpretation of Spectrum:

  • The spectrum of a rectangular pulse is a sinc function.
  • The main lobe of the sinc function is centered at omega = 0 (DC).
  • The width of the main lobe (from the first zero crossing on one side to the first zero crossing on the other) is inversely proportional to the pulse duration T. Specifically, the first zero crossing occurs at omega = 2*pi / T.
  • Key Insight: A wider pulse in the time domain (larger T) results in a narrower main lobe in the frequency domain, meaning its energy is concentrated in a smaller bandwidth. Conversely, a narrower pulse in time (smaller T) spreads its energy over a wider range of frequencies. This vividly demonstrates the inverse relationship between time duration and bandwidth.

Detailed Explanation

A rectangular pulse is a basic wave that has a flat shape for a certain duration (T) and is zero elsewhere. This means it has a height of 1 for the time it is active and zero when inactive. When we take its Fourier Transform (FT), we analyze its frequency content. The FT of the rectangular pulse results in a sinc function. The sinc function describes how the pulse's duration relates inversely to the bandwidth of its frequency representation. For instance, if the pulse lasts longer (increased T), its frequency representation becomes narrower, indicating that it primarily contains lower frequencies.

Examples & Analogies

Imagine turning on a light in a room for a short duration. When the light is on, it is very bright (the rectangular pulse), and when it's off, the room is dark (zero). If you keep the light on longer, the brightness is concentrated in that brief moment (short frequency range) compared to if you flicked the light on and off quickly, which would spread the brightness over a longer duration (wider frequency range).

Unit Impulse Function

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4.4.2 Unit Impulse Function (delta(t))

Time Domain Definition:

The Dirac delta function, delta(t), is an idealized signal (not a regular function) with infinite amplitude at t=0, zero amplitude elsewhere, and an area of 1.

Derivation of FT:

X(jomega) = Integral from -infinity to +infinity of (delta(t) * e^(-j * omega * t) dt)
Using the sifting property of the impulse function (Integral of f(t)delta(t-t0) dt = f(t0)), with t0 = 0 and f(t) = e^(-jomegat), we get:

Fourier Transform Result:

X(j*omega) = e^(j * omega * 0) = 1

Interpretation of Spectrum:

The Fourier Transform of a unit impulse is a constant value of 1 across all frequencies. This means that the impulse function contains all frequencies with equal amplitude and zero phase shift. This is consistent with its time-domain nature: a perfectly sharp, instantaneous event requires an infinite range of frequency components to be accurately represented.

Detailed Explanation

The unit impulse function, represented by delta(t), is a unique mathematical construction that represents an instantaneous event at a single point in time (t=0). When we calculate the Fourier Transform of the impulse, we find that it outputs a constant value of 1 across all frequencies. This indicates the impulse function includes every possible frequency since it happens instantaneously. Therefore, fundamentally, the impulse contains all frequencies required to represent any signal.

Examples & Analogies

Think of a sharp clap. It's a quick, sudden sound (the impulse) that generates a broad range of frequencies all at once. You can hear all kinds of tones in that single clap, much like how the delta function encompasses all frequency ranges in its representation.

Unit Step Function

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4.4.3 Unit Step Function (u(t))

Time Domain Definition:

The unit step function, u(t), is 0 for t < 0 and 1 for t >= 0.

Derivation of FT (Conceptual/Property-Based):

  • The unit step function is not absolutely integrable, so its Fourier Transform is defined using generalized functions (specifically, the impulse function).
  • We know that the derivative of the unit step is the unit impulse: d/dt u(t) = delta(t).
  • Using the Differentiation in Time property: F{d/dt u(t)} = j*omega * F{u(t)}.
  • Since F{delta(t)} = 1, we have: 1 = j*omega * F{u(t)}.
  • Solving for F{u(t)} yields F{u(t)} = 1 / (j*omega). However, this misses the DC component.
  • A more rigorous approach accounts for the average value (DC component) of u(t), which is 1/2 over infinite time. The full derivation usually involves analyzing u(t) as the limit of a decaying exponential or using properties.

Fourier Transform Result:

X(jomega) = (1 / (jomega)) + pi * delta(omega)

Interpretation of Spectrum:

  • The term (1 / (j*omega)) represents the frequency content associated with the step change. It shows that higher frequencies are attenuated (as omega increases, 1/omega decreases).
  • The term pi * delta(omega) represents the DC component (zero frequency component). The unit step function has an average value of 1/2 over infinite time, which contributes to the impulse at DC in the frequency domain.

Detailed Explanation

The unit step function is a fundamental signal that changes from zero to one abruptly at time t=0. Calculating its Fourier Transform can be intricate since it's not absolutely integrable due to its defined behavior over time. We derive its Fourier Transform by recognizing that its derivative is the Dirac delta function. Through its transform, we extract insights about the contributions of different frequency componentsβ€”specifically distinguishing between the frequency change represented and its constant (DC) contribution derived from the step's nature.

Examples & Analogies

Imagine a light switch. When you turn it on, the light instantly turns on from dark (0) to bright (1). This immediate change (the step) happens exactly at the moment you flip the switch. When describing how this switch impacts the overall lighting scenario, we need to consider both the change itself and the steady light it creates after turning on (the constant light). This is analogous to our Fourier Transform addressing not just the frequency change but also the DC level maintained afterward.

Exponential Signals

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4.4.4 Exponential Signals

Real Exponential (Decaying, e^(-at)u(t) for a > 0):

  • Time Domain Definition: x(t) = e^(-at)u(t). This signal starts at t=0 and decays exponentially as t increases.
  • Derivation of FT:
    X(jomega) = Integral from t = 0 to t = +infinity of (e^(-at) * e^(-j * omega * t) dt)
    X(jomega) = Integral from t = 0 to t = +infinity of (e^(-(a + j*omega) * t) dt)
    Solving this integral (which is a standard improper integral).
  • Fourier Transform Result:
    X(jomega) = 1 / (a + jomega)
  • Interpretation of Spectrum: This is a complex spectrum. The magnitude |X(j*omega)| = 1 / sqrt(a^2 + omega^2) shows that the spectrum is highest at omega=0 (DC) and rolls off as frequency increases. This is consistent with a decaying signal that has more low-frequency content.

Complex Exponential (e^(jomega0t)):

  • Time Domain Definition: x(t) = e^(jomega0t). This is an infinitely long, pure complex sinusoid.
  • Derivation of FT (Conceptual/Property-Based): This signal is not absolutely integrable, so its FT is defined using generalized functions (impulses), usually by using the duality property or by considering it as the inverse FT of a single impulse.
  • Fourier Transform Result:
    X(jomega) = 2pi * delta(omega - omega0)
  • Interpretation of Spectrum: A pure complex exponential in the time domain corresponds to a single impulse in the frequency domain located exactly at its angular frequency (omega0). This means the signal consists of only one frequency component, as expected.

Detailed Explanation

In examining exponential signals, we focus first on real exponential decay functions, typically defined to start at maximum value and gradually reduce over time. The Fourier Transform for these signals shows that they maintain higher amplitudes at lower frequencies, because their decay reduces the high-frequency content significantly. In contrast, a complex exponential represents a pure wave at a specific frequency without decay, and its Fourier Transform reveals not a spread of frequencies but a concentrated impulse at that unique frequency, indicating it possesses only that one frequency component.

Examples & Analogies

Think of a running faucet. At first, the water (real exponential decay) flows out quickly then gradually decreases until it stops, representing a decaying signal. Conversely, consider a continuously flowing springβ€”we hear a constant humming sound (complex exponential) at a steady pitch without fading, showing it’s comprised of a singular frequency. These examples highlight the contrast between signals that fade over time and those that maintain a steady output over time.

Sinusoidal Signals

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4.4.5 Sinusoidal Signals (cos(omega0t) and sin(omega0t))

  • Using Euler's Formula and Linearity: We derive the FT of real sinusoids by expressing them as a sum of complex exponentials using Euler's formula and then applying the linearity property and the FT of a complex exponential.

Cosine (cos(omega0*t)):

  • Time Domain Definition: x(t) = cos(omega0t) = (1/2) * (e^(jomega0t) + e^(-jomega0*t))
  • Derivation of FT:
    F{cos(omega0t)} = F{(1/2) * e^(jomega0t)} + F{(1/2) * e^(-jomega0t)}
    (by linearity)
    = (1/2) * [2pi * delta(omega - omega0)] + (1/2) * [2*pi * delta(omega - (-omega0))]
  • Fourier Transform Result:
    X(j*omega) = pi * [delta(omega - omega0) + delta(omega + omega0)]
  • Interpretation of Spectrum: The spectrum of a cosine wave consists of two impulses, one at positive frequency (+omega0) and one at negative frequency (-omega0), each with a strength of pi. This confirms that a real cosine wave is composed of two complex exponentials rotating in opposite directions.

Sine (sin(omega0*t)):

  • Time Domain Definition: x(t) = sin(omega0t) = (1/(2j)) * (e^(jomega0t) - e^(-jomega0*t))
  • Derivation of FT: Similar to cosine, applying linearity.
  • Fourier Transform Result:
    X(jomega) = jpi * [delta(omega + omega0) - delta(omega - omega0)]
  • Interpretation of Spectrum: The spectrum of a sine wave also consists of two impulses at +omega0 and -omega0, but with opposite signs and multiplied by 'j'. This means the components are 90 degrees out of phase compared to the cosine components, which is consistent with the sine and cosine relationship.

Detailed Explanation

Sinusoidal signals are foundational in signal processing. To derive their Fourier Transforms, we leverage Euler's formula, which relates sinusoidal functions to complex exponentials. For cosines, their Fourier Transform yields two impulses in the frequency domain, symbolizing the presence of both positive and negative frequency components. Sines, likewise, produce similar impulses but exhibit a phase difference, providing insights necessary for understanding oscillating systems in both theoretical and practical applications.

Examples & Analogies

Imagine tuning into a radio station. When you hear a clear pitch (cosine wave), it resonates at a specific frequency but is represented through two harmonics (impulses) that move in opposite directions. Meanwhile, the distortion you occasionally hear (sine wave) might represent an out-of-phase condition where the sound waves collide, producing an alternative experience. This illustrates how both sine and cosine functions underlie the signals we interact with in everyday devices.

Definitions & Key Concepts

Learn essential terms and foundational ideas that form the basis of the topic.

Key Concepts

  • Rectangular Pulse: Represents a clear time-defined waveform with its energy distributed in frequency.

  • Unit Impulse Function: A fundamental representation in time that encapsulates all frequencies equally.

  • Unit Step Function: Captures the transition from one state to another while indicating frequency response.

  • Exponential Signals: Show how decay affects the frequency components, with the real and complex forms revealing unique properties.

Examples & Real-Life Applications

See how the concepts apply in real-world scenarios to understand their practical implications.

Examples

  • The Fourier Transform of a rectangular pulse results in a sinc function, illustrating the inverse relationship between pulse duration and bandwidth.

  • For the Dirac delta function, its Fourier Transform yields a constant magnitude across all frequencies, indicating all frequency components are present.

  • The Fourier Transform of the unit step function includes both a frequency term and a delta term, representing its continuous contribution across frequencies.

Memory Aids

Use mnemonics, acronyms, or visual cues to help remember key information more easily.

🎡 Rhymes Time

  • Rectangular pulse, nice and neat, its transform's a sinc, can't be beat!

πŸ“– Fascinating Stories

  • Imagine a light switch that turns on instantly. This is a unit impulseβ€”a flick that captures all possible energies at once!

🧠 Other Memory Gems

  • For the unit step, remember 'U goes up, but isn't down; in frequencies, it makes waves abound.'

🎯 Super Acronyms

R.U.E. - Where R means Rectangular pulse, U means Unit impulse, and E means Exponential signals.

Flash Cards

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Glossary of Terms

Review the Definitions for terms.

  • Term: Rectangular Pulse

    Definition:

    A signal that has a constant amplitude of 1 for a specified duration T and 0 elsewhere.

  • Term: Fourier Transform

    Definition:

    A mathematical transformation that converts a time-domain signal into its frequency-domain representation.

  • Term: sinc Function

    Definition:

    A mathematical function defined as sinc(x) = sin(Ο€x)/(Ο€x), representing the spectral content of a rectangular pulse.

  • Term: Unit Impulse Function (delta(t))

    Definition:

    An idealized function that represents an instantaneous impulse at t=0, with importance in frequency analysis.

  • Term: Unit Step Function (u(t))

    Definition:

    A signal that transitions from 0 to 1 at t=0, used to represent signals that start at a specified time.

  • Term: Exponential Signal

    Definition:

    A signal characterized by an exponential decay or growth, significantly affecting its frequency representation.

  • Term: Complex Exponential

    Definition:

    A sinusoidal signal represented in the form e^(jωt), related to frequency components.