7.7 - Proof (for n=1)
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Introduction to Laplace Transforms
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Hello class, today we’re diving into Laplace Transforms! Who can tell me what a Laplace Transform does?
Is it like translating functions from the time domain to the frequency domain?
Exactly! The basic definition is that it transforms a function f(t) defined for t ≥ 0 to the s-domain. We represent this as L{f(t)} = F(s).
Could you explain what the integral looks like?
Sure! The transformation is defined by the integral: ∫ e^(-st) f(t) dt from 0 to infinity. It simplifies many differential equations!
That sounds really useful! What happens when we multiply by tn?
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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Now, if we have L{f(t)} = F(s), what do you think L{tn f(t)} corresponds to?
Is it the derivative of F(s) with respect to s?
Absolutely! It’s actually the nth derivative. So, L{tn f(t)} = (-1)^n (d^n/ds^n) F(s).
Can you explain why we have that alternating sign?
The sign alternates because of the repeated differentiation. The first derivative gives a negative sign, and that pattern continues with each differentiation.
And does this apply to all time-domain functions?
Good question! The function must be piecewise continuous and of exponential order.
Proof for n=1
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Let’s explore the proof for n=1. Who can summarize what L{tf(t)} equals?
It equals the negative derivative of F(s) with respect to s!
Exactly! We have L{tf(t)} = - (dF(s)/ds). Let's walk through the calculation together.
What about applying this to examples?
Yes! Let’s take L{t * sin(at)}. What’s the base we start from?
L{sin(at)} = a / (s² + a²).
Correct! Now applying the derivative gives L{t * sin(at)} = - (d/ds)(1 / (s² + a²)).
Applications of Multiplication by tn
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Now let’s look at the applications. Any thoughts on where we might use this multiplication property?
In control systems to model time delays!
Exactly, and it’s also used in electrical engineering and mechanical vibrations to deal with polynomial forcing functions!
How about in signal processing?
Great thought! It helps with time-domain convolution and modulation.
What do we need to remember when applying this property?
Always apply the formula after computing L{f(t)} and be careful with rational function differentiation.
Introduction & Overview
Read summaries of the section's main ideas at different levels of detail.
Quick Overview
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.
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Definition of L{f(t)}
Chapter 1 of 5
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Chapter Content
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
Chapter 2 of 5
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Chapter Content
Now, consider: ∞ L{tf(t)}=∫e−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)
Chapter 3 of 5
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Chapter Content
We take the derivative of F(s): dF(s) d ∞ ∞ d ∞ = ∫e−stf(t)dt=∫ (e−st )f(t)dt=−∫te−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)}
Chapter 4 of 5
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Chapter Content
So: dF(s) L{tf(t)}=− 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
Chapter 5 of 5
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Chapter Content
This generalizes to: L{tnf(t)}=¿
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.
Key Concepts
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Multiplication by tn: This property allows for easier manipulation of functions when they are multiplied by time powers.
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s-Domain Differentiation: Taking derivatives of functions in the s-domain can simplify solving differential equations related to time-domain problems.
Examples & Applications
Example 1: Find L{t * sin(at)}; L{sin(at)} = a / (s² + a²); thus L{t * sin(at)} = - (d/ds)(a / (s² + a²)).
Example 2: Find L{t² * e^(at)}; L{e^(at)} = 1 / (s - a); thus L{t² * e^(at)} = (d²/ds²)(1 / (s - a)).
Memory Aids
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Rhymes
To find L{tn f(t)}, don't let it flit, just take derivatives and you’re all set!
Stories
Imagine a function on a journey to the s-domain, bumping into differentiation every time it picks up speed (time).
Memory Tools
D-ifferentiate, A-lternating sign, N-ow you’ve got L{tn f(t)} in line (DAN).
Acronyms
DAN - Differentiate and Alternating for N-th derivatives.
Flash Cards
Glossary
- Laplace Transform
A mathematical transformation that converts a function in the time domain into a function in the complex frequency domain.
- sdomain
The domain used in Laplace Transforms, representing complex frequency (s) rather than time (t).
- Piecewise Continuous
A property of functions where they are continuous except for a finite number of discontinuities.
- Exponential Order
A property of functions where they exhibit growth bounded by an exponential function as t approaches infinity.
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