Proof (for n=1) - 7.7 | 7. Multiplication by tn (Power of t) | Mathematics - iii (Differential Calculus) - Vol 1
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Interactive Audio Lesson

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

Introduction to Laplace Transforms

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0:00
Teacher
Teacher

Hello class, today we’re diving into Laplace Transforms! Who can tell me what a Laplace Transform does?

Student 1
Student 1

Is it like translating functions from the time domain to the frequency domain?

Teacher
Teacher

Exactly! The basic definition is that it transforms a function f(t) defined for t β‰₯ 0 to the s-domain. We represent this as L{f(t)} = F(s).

Student 2
Student 2

Could you explain what the integral looks like?

Teacher
Teacher

Sure! The transformation is defined by the integral: ∫ e^(-st) f(t) dt from 0 to infinity. It simplifies many differential equations!

Student 3
Student 3

That sounds really useful! What happens when we multiply by tn?

Teacher
Teacher

Great question! Multiplying by tn leads us to the multiplication property of Laplace Transforms. Let’s explore that!

Multiplication by tn Property

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0:00
Teacher
Teacher

Now, if we have L{f(t)} = F(s), what do you think L{tn f(t)} corresponds to?

Student 4
Student 4

Is it the derivative of F(s) with respect to s?

Teacher
Teacher

Absolutely! It’s actually the nth derivative. So, L{tn f(t)} = (-1)^n (d^n/ds^n) F(s).

Student 1
Student 1

Can you explain why we have that alternating sign?

Teacher
Teacher

The sign alternates because of the repeated differentiation. The first derivative gives a negative sign, and that pattern continues with each differentiation.

Student 3
Student 3

And does this apply to all time-domain functions?

Teacher
Teacher

Good question! The function must be piecewise continuous and of exponential order.

Proof for n=1

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0:00
Teacher
Teacher

Let’s explore the proof for n=1. Who can summarize what L{tf(t)} equals?

Student 2
Student 2

It equals the negative derivative of F(s) with respect to s!

Teacher
Teacher

Exactly! We have L{tf(t)} = - (dF(s)/ds). Let's walk through the calculation together.

Student 4
Student 4

What about applying this to examples?

Teacher
Teacher

Yes! Let’s take L{t * sin(at)}. What’s the base we start from?

Student 3
Student 3

L{sin(at)} = a / (sΒ² + aΒ²).

Teacher
Teacher

Correct! Now applying the derivative gives L{t * sin(at)} = - (d/ds)(1 / (sΒ² + aΒ²)).

Applications of Multiplication by tn

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0:00
Teacher
Teacher

Now let’s look at the applications. Any thoughts on where we might use this multiplication property?

Student 1
Student 1

In control systems to model time delays!

Teacher
Teacher

Exactly, and it’s also used in electrical engineering and mechanical vibrations to deal with polynomial forcing functions!

Student 2
Student 2

How about in signal processing?

Teacher
Teacher

Great thought! It helps with time-domain convolution and modulation.

Student 4
Student 4

What do we need to remember when applying this property?

Teacher
Teacher

Always apply the formula after computing L{f(t)} and be careful with rational function differentiation.

Introduction & Overview

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

Quick Overview

This section explains how multiplying a function by a power of time relates to differentiating its Laplace Transform.

Standard

Exploring the multiplication by tn property in Laplace Transforms, this section shows that the Laplace Transform of tn multiplied by a function can be calculated by differentiating the Laplace Transform of the original function. Additionally, it includes proofs, examples, and applications relevant to the property.

Detailed

Detailed Summary

In this section, we explore the multiplication by tn property in Laplace Transforms, a foundational concept important for manipulating time-domain functions through algebraic methods in the s-domain. Given a function f(t), the Laplace Transform, denoted L{f(t)} = F(s), converts this function into the s-domain through the integral transformation. When this function is multiplied by a power of time, specifically tn, the relationship takes the form:

  • L{tnf(t)} = (-1)^n (d^n/ds^n) F(s)

Significance

This relation highlights that the act of multiplying a time-domain function by a power of time corresponds to differentiating its Laplace Transform n times with respect to s, while introducing an alternating sign factor (-1)^n. The section provides detailed proof for the case when n=1 where we inspect the transformation L{tf(t)} and show it works out to L{tf(t)} = - (d/ds) F(s). Furthermore, examples provided illustrate how this principle applies in practical scenarios, such as calculating the Laplace Transform of products involving time and sine or exponential functions. Lastly, applications in control systems and signal processing are noted, emphasizing its practical importance.

Audio Book

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Definition of L{f(t)}

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Let L{f(t)}=F(s)

Detailed Explanation

In this part of the proof, we start by noting the relationship between the Laplace Transform of a function f(t) and its representation in the s-domain, denoted as F(s). This states that if you take the Laplace Transform of the function f(t), you get F(s). This is a fundamental starting point for further calculations.

Examples & Analogies

Think of L{f(t)} as a recipe for a dish. Here, f(t) is the original dish made from various ingredients (like vegetables, meat, and spices) and L{f(t)} provides the 'instruction' on how to prepare it, resulting in a delightful finished product F(s) that represents how it tastes.

Setting Up the Integral

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Now, consider: ∞ L{tf(t)}=∫eβˆ’sttf(t)dt 0

Detailed Explanation

Next, we focus on how to calculate the Laplace Transform of the function multiplied by t, that is, tf(t). We express this as an integral from 0 to infinity of e^(-st) multiplied by tf(t). This integral setup is crucial because it helps us relate time-domain functions to their transforms in the s-domain.

Examples & Analogies

Imagine you are measuring the impact of an activity over time, like how far a car travels (tf(t)) when factoring in the time itself. The integral represents collecting all those measurements from the start of the journey (0) to the finish (infinity).

Derivation of F(s)

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We take the derivative of F(s): dF(s) d ∞ ∞ d ∞ = ∫eβˆ’stf(t)dt=∫ (eβˆ’st )f(t)dt=βˆ’βˆ«teβˆ’stf(t)dt 0 0 0

Detailed Explanation

Here, we differentiate F(s) with respect to s. This leads us to break down the original integral into components and ultimately shows another integral that involves tf(t). This step is essential in proving how the multiplication by t translates into an operation in the s-domain through differentiation.

Examples & Analogies

Think of differentiation like adjusting the nozzle of a hose to control the water flow. By changing the flow (the derivative), you can control how far and how fast the water (the function) travels. This adjustment allows you to model more complex functions accurately.

Final Expression for L{tf(t)}

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So: dF(s) L{tf(t)}=βˆ’ ds

Detailed Explanation

By continuing through our calculations, we conclude that the Laplace Transform of tf(t) is simply the negative derivative of F(s) with respect to s. This negation is an important part of the relationship we have established through our earlier steps.

Examples & Analogies

This step can be likened to discovering that pressing down on a claim counter (the derivative) gives you a negative return on investment. The process of finding the Laplace Transform is like seeing how altering your inputs affects your outputs, leading to new insights.

Generalization to Higher n

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This generalizes to: L{tnf(t)}=ΒΏ

Detailed Explanation

Finally, we note that this process can be extended. The main takeaway is that multiplying by tn corresponds to taking the n-th derivative of F(s) and coupling that with a specific factor (the sign is influenced by how many times we differentiate). This generalization is crucial and forms the base for solving more complicated problems using Laplace Transforms.

Examples & Analogies

Consider this as a guideline for building a larger structure. If n has to do with the number of stories in a building, each level represents a new layer of complexity that can be handled with a consistent approach (like taking derivatives) ensuring that the building remains stable and functional.

Definitions & Key Concepts

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

Key Concepts

  • Multiplication by tn: This property allows for easier manipulation of functions when they are multiplied by time powers.

  • s-Domain Differentiation: Taking derivatives of functions in the s-domain can simplify solving differential equations related to time-domain problems.

Examples & Real-Life Applications

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

Examples

  • Example 1: Find L{t * sin(at)}; L{sin(at)} = a / (sΒ² + aΒ²); thus L{t * sin(at)} = - (d/ds)(a / (sΒ² + aΒ²)).

  • Example 2: Find L{tΒ² * e^(at)}; L{e^(at)} = 1 / (s - a); thus L{tΒ² * e^(at)} = (dΒ²/dsΒ²)(1 / (s - a)).

Memory Aids

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

🎡 Rhymes Time

  • To find L{tn f(t)}, don't let it flit, just take derivatives and you’re all set!

πŸ“– Fascinating Stories

  • Imagine a function on a journey to the s-domain, bumping into differentiation every time it picks up speed (time).

🧠 Other Memory Gems

  • D-ifferentiate, A-lternating sign, N-ow you’ve got L{tn f(t)} in line (DAN).

🎯 Super Acronyms

DAN - Differentiate and Alternating for N-th derivatives.

Flash Cards

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Glossary of Terms

Review the Definitions for terms.

  • Term: Laplace Transform

    Definition:

    A mathematical transformation that converts a function in the time domain into a function in the complex frequency domain.

  • Term: sdomain

    Definition:

    The domain used in Laplace Transforms, representing complex frequency (s) rather than time (t).

  • Term: Piecewise Continuous

    Definition:

    A property of functions where they are continuous except for a finite number of discontinuities.

  • Term: Exponential Order

    Definition:

    A property of functions where they exhibit growth bounded by an exponential function as t approaches infinity.