Systematic Cases for Denominator Roots (Poles) - 5.2.1.3 | Module 5: Laplace Transform Analysis of Continuous-Time Systems | Signals and Systems
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5.2.1.3 - Systematic Cases for Denominator Roots (Poles)

Practice

Interactive Audio Lesson

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

Distinct Real Poles

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0:00
Teacher
Teacher

Today, we're going to discuss how to handle distinct real poles in the context of partial fraction expansion. Can anyone tell me what we mean by distinct real poles?

Student 1
Student 1

Are they simply poles that are different from each other on the real axis?

Teacher
Teacher

Exactly! If we have a denominator that can be factored into distinct real roots, we express our function in the form of sums of simpler fractions: K1 / (s - p1) + K2 / (s - p2) + ... Can anyone think of a method we can use to find these coefficients K_i?

Student 2
Student 2

The cover-up method! We multiply by (s - pi) and evaluate at s = pi.

Teacher
Teacher

Right! That helps get those coefficients quickly. Also remember, the alternative is to equate coefficients after cross-multiplication. So, practice this method: if you have X(s) = 10 / (s - 2)(s - 3), how do we find K1 and K2?

Student 3
Student 3

We can say X(s) = K1 / (s - 2) + K2 / (s - 3) and cover up to solve for each K!

Teacher
Teacher

Excellent! Remember, distinct poles lead to straightforward sections in your inverse transformation process. To recap, distinct real poles are represented as sums of simpler fractions, and we can use either the cover-up method or coefficient comparison to find coefficients.

Repeated Real Poles

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Teacher
Teacher

Next, let's discuss the situation when we encounter repeated real poles in our partial fraction expansion. What does that mean, and how does it change our PFE structure?

Student 4
Student 4

It means one of the poles has a multiplicity! So, instead of just K1 and K2, we have additional terms like A2 / (s - p1)^2.

Teacher
Teacher

Exactly! We write X(s) = A1 / (s - p1) + A2 / (s - p1)^2 + ... An / (s - p1)^n. Can anyone suggest how we find coefficients for these terms?

Student 1
Student 1

For the highest power, we can still use the cover-up method, right?

Teacher
Teacher

Correct! For the coefficient of the highest power A_n, we can cover up as we did before. For the lower powers, though, we need to utilize derivatives. Who can remember how we find A_k through derivatives?

Student 2
Student 2

We can use A_k = [1 / (n-k)!] * (d^(n-k)/ds^(n-k) of [(s - p1)^n * X(s)]) evaluated at s = p1.

Teacher
Teacher

Great job! Remember this process for repeated poles can get lengthy, so be patient and systematic. To recap, repeated poles require careful attention with coefficients derived from derivatives and the cover-up method.

Complex Conjugate Poles

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0:00
Teacher
Teacher

Finally, let’s discuss complex conjugate poles. Who can explain how these differ from real poles in terms of PFE?

Student 3
Student 3

Complex poles always come in pairs, right? So we have to combine them when forming the PFE.

Teacher
Teacher

Exactly! You can treat them as complex coefficients, or a more preferred method is to use a single quadratic term: (As + B) / (s^2 + 2*alpha*s + alpha^2 + beta^2). This simplifies your inverse transform process. Can anyone tell me why this is preferable?

Student 4
Student 4

Because it directly relates to damped sinusoidal outputs in the time-domain!

Teacher
Teacher

That’s right! When you understand that, recognizing damped sinusoids will become easier. Remember, pull out the real-coefficient expression. So for complex conjugate poles, we often simplify the process greatly. To summarize, complex conjugates can significantly ease the transition back to the time domain.

Introduction & Overview

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

Quick Overview

This section outlines the systematic approach to performing partial fraction expansion based on the nature of the poles in a denominator polynomial.

Standard

In this section, we explore different cases for poles in the denominator of rational functions encountered during inverse Laplace transformation. The methods differ based on whether the poles are distinct real, repeated real, or complex conjugates, and knowing these cases is essential for accurately applying the Inverse Laplace Transform.

Detailed

Systematic Cases for Denominator Roots (Poles)

In inverse Laplace transformation, the nature of the poles of the denominator polynomial determines the appropriate method for partial fraction expansion (PFE). Understanding these systematic cases is crucial for decomposing a complex rational function into simpler terms, allowing for an easier inverse transformation.

1. Case 1: Distinct Real Poles

If the denominator can be factored into distinct real roots, the PFE is expressed as:

X(s) = K1 / (s - p1) + K2 / (s - p2) + ... + Kn / (s - pn)

The coefficients (K_i) can be found using the cover-up method or by equating coefficients after cross-multiplication.

2. Case 2: Repeated Real Poles

For repeated real roots (p1 with multiplicity n), the PFE is structured as:

X(s) = A1 / (s - p1) + A2 / (s - p1)^2 + ... + An / (s - p1)^n

The coefficients can be found using derivatives in conjunction with the cover-up method for the highest coefficient.

3. Case 3: Complex Conjugate Poles

Complex conjugate poles can be managed in two ways: treating them as distinct poles or combining them into a single quadratic term:

(As + B) / (s^2 + 2alphas + alpha^2 + beta^2)

This allows a direct relation to damped oscillations in the inverse transform.

Having a clear understanding of these cases ensures accurate application of PFE, facilitating a smoother transition from the s-domain back to the time-domain functions.

Audio Book

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Case 1: Distinct Real Poles

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If the denominator D(s) can be factored into distinct real roots like (s - p1)(s - p2)...(s - pn), then the PFE takes the form:

X(s) = K1 / (s - p1) + K2 / (s - p2) + ... + Kn / (s - pn

Finding Coefficients (Ki): The most common technique is the 'cover-up method' (Heaviside method). For each coefficient Ki, multiply X(s) by the factor (s - pi) and then evaluate the resulting expression at s = pi.

Ki = [(s - pi) * X(s)] evaluated at s = pi.

Alternatively, coefficients can be found by cross-multiplication, bringing all terms to a common denominator, and then equating coefficients of like powers of 's' in the numerator.

Detailed Explanation

In this case, when we have distinct real poles, we can factor the denominator into linear terms. Each term corresponds to a pole in the partial fraction expansion (PFE). The structure of the PFE allows us to express the rational function as a sum of simpler fractions, where each fraction represents a pole. For each distinct real pole, we find a coefficient using the cover-up method, which involves multiplying the entire function by (s - p_i) and then evaluating the result at s = p_i. This process gives us the necessary constants (K_i) that define the contribution of each pole to the overall transform. Alternatively, coefficients can be determined by manipulating the terms to isolate each component, providing a different method to arrive at the final equation.

Examples & Analogies

Imagine you are assembling a puzzle where each distinct piece represents a different pole. Just as you need to identify where each piece fits in the larger picture, in the mathematical process, we identify how each pole contributes to the overall system. By using the cover-up method, you effectively isolate each piece to understand its role in the complete imageβ€”the final transformed function.

Case 2: Repeated Real Poles

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If the denominator D(s) has a repeated real root, for example, (s - p1) raised to the power of n (meaning p1 is a root of multiplicity n), then the PFE includes a series of terms for that pole:

X(s) = A1 / (s - p1) + A2 / (s - p1)^2 + ... + An / (s - p1)^n + ...

(plus terms for other distinct poles).

Finding Coefficients (Ak): For the highest power term (An), the cover-up method still works: An = [(s - p1)^n * X(s)] evaluated at s = p1. For lower power terms, derivatives are required:

Ak = [1 / (n - k)!] * (d raised to the power of (n-k) / d s raised to (n-k)) of [(s - p1)^n * X(s)] evaluated at s = p1.

This can be tedious. Often, a combination of the cover-up method for the highest power and equating coefficients after cross-multiplication for other terms is more practical.

Detailed Explanation

When encountering repeated real poles, the denominator cannot be factored into simple linear terms, as in the previous case. Instead, each repetition introduces a new term in the PFE. For a pole of multiplicity n, we represent this as a series of fractions, with each term corresponding to a different power of (s - p_1). The cover-up method can still be applied for the highest order term, while for the lower-order terms, we need to take derivativesβ€”this is akin to peeking beneath the surface to extract deeper information about the function. Despite being more tedious, established mathematical techniques help to ensure we correctly identify each coefficient's contribution.

Examples & Analogies

Think of it like a tree with multiple trunks that are all connected at the ground level. Each trunk represents a repeated pole, and the branches (fractions in the PFE) extend from each trunk. As you identify that the trunk continues to split, you explore further into the network of branches for better understanding. In this case, using derivatives helps uncover the deeper intricacies of how each trunk influences the tree's expansion.

Case 3: Complex Conjugate Poles

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For real-coefficient polynomials, complex roots always appear in conjugate pairs. If D(s) has a pair like (s - (alpha + jbeta))(s - (alpha - jbeta)), which expands to a quadratic term (s^2 + 2 * alpha * s + alpha^2 + beta^2), the corresponding terms in the PFE can be handled in two ways:

  • Method A (Complex Coefficients): Treat them as distinct poles and use the distinct pole method. This will yield complex coefficients that are also conjugates. Inverse transforming these will combine to form real-valued damped sinusoidal terms.
  • Method B (Real Coefficients - Preferred): Use a single quadratic term in the PFE with real coefficients:

(As + B) / (s^2 + 2alpha*s + alpha^2 + beta^2)

This form directly corresponds to inverse transforms involving damped sinusoids (e raised to the power of (alphat) * cos(betat + phi) or e raised to the power of (alphat) * sin(betat)). To find A and B, typically equate coefficients after cross-multiplication or use a combination of evaluating X(s) at specific 's' values (e.g., s=0 or s=1) and equating coefficients.

Detailed Explanation

When dealing with complex conjugate poles, the approach slightly differs since they can be conveniently represented as a single quadratic term. Here, we have two methods: the first is to treat each complex pole separately and apply the standard methods to find their respective coefficients. The second, often preferred method, involves realizing that the quadratic form suffices to capture the contributions of these poles effectively. By using real coefficients, we can directly tie our results back to familiar sinusoidal functionsβ€”a major advantage in applications like control systems or signal processing.

Examples & Analogies

Imagine you are mixing two colors that are complementary. Individually, they can represent different tones and hues (the complex poles), but when blended into a single shade (the quadratic term), they create a harmonious color that reflects both qualities together. This blending resonates with how complex conjugate poles work together to form unified oscillatory behavior in systems, resulting in outputs that exhibit both amplitude modulation and sinusoidal patterns.

Definitions & Key Concepts

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

Key Concepts

  • Partial Fraction Expansion (PFE): A method for breaking down rational functions based on pole types.

  • Distinct Real Poles: Represent unique points on the real axis where the function can be decomposed into simpler fractions.

  • Repeated Real Poles: Indicate multiplicity, adding complexity to the decomposition process.

  • Complex Conjugate Poles: Pairs of complex roots that influence oscillatory behavior in inverse transformations.

Examples & Real-Life Applications

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

Examples

  • Example of distinct real poles: For X(s) = 10 / ((s-1)(s-2)), using the cover-up method leads to K1 = 5, K2 = 5.

  • Example of repeated real poles: X(s) = 10 / ((s-1)^2)(s-2) can be decomposed into A1/(s-1) + A2/(s-1)^2 + K/(s-2).

Memory Aids

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

🎡 Rhymes Time

  • To find K with cover-up so neat, just multiply and find the treat.

πŸ“– Fascinating Stories

  • Imagine a tree with distinct branches. Each branch represents a unique pole, and to find the path to the fruit (the coefficient), we cover the other branches and just examine the one we want.

🧠 Other Memory Gems

  • For real poles, remember 'D' for distinct and 'R' for repeated - distinct is a single path, repeated takes a longer route.

🎯 Super Acronyms

PFE - Poles Facilitate Expansion. Always remember, knowing the poles helps break down fractions.

Flash Cards

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Glossary of Terms

Review the Definitions for terms.

  • Term: Partial Fraction Expansion (PFE)

    Definition:

    A method of expressing a rational function as a sum of simpler fractions based on its poles.

  • Term: Distinct Real Poles

    Definition:

    Poles that are different and located on the real axis in the complex s-plane.

  • Term: Repeated Real Poles

    Definition:

    Poles that appear more than once in the factorization of a polynomial, indicating higher multiplicity.

  • Term: Complex Conjugate Poles

    Definition:

    Pairs of complex roots that arise from real-coefficient polynomials, typically affecting oscillatory behavior.