Laplace Transform in Solving Differential Equations - 15.14 | 15. Fourier Integral to Laplace Transforms | Mathematics (Civil Engineering -1)
K12 Students

Academics

AI-Powered learning for Grades 8–12, aligned with major Indian and international curricula.

Professionals

Professional Courses

Industry-relevant training in Business, Technology, and Design to help professionals and graduates upskill for real-world careers.

Games

Interactive Games

Fun, engaging games to boost memory, math fluency, typing speed, and English skills—perfect for learners of all ages.

15.14 - Laplace Transform in Solving Differential Equations

Enroll to start learning

You’ve not yet enrolled in this course. Please enroll for free to listen to audio lessons, classroom podcasts and take practice test.

Practice

Interactive Audio Lesson

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

Introduction to Laplace Transform

Unlock Audio Lesson

0:00
Teacher
Teacher

Today, we'll discuss how the Laplace Transform helps us solve differential equations. Can anyone tell me what a differential equation is?

Student 1
Student 1

Isn't a differential equation an equation that involves derivatives?

Teacher
Teacher

Exactly, great job! The Laplace Transform converts those derivatives into algebraic equations, making them much easier to work with. Remember, the key concept here is transforming complexity into simplicity.

Student 2
Student 2

So, how does that transformation actually work?

Teacher
Teacher

That's a good question! The Laplace Transform takes a function defined in the time domain and translates it into the frequency domain. We express this with: $$ F(s) = L \{ f(t) \} = \int_0^{\infty} e^{-st} f(t) dt $$.

Student 3
Student 3

What do 's' and 't' represent in this equation?

Teacher
Teacher

't' is the time variable, while 's' is a complex number used as a parameter in the transform. This allows us to manipulate the functions more flexibly.

Teacher
Teacher

In summary, the Laplace Transform is instrumental for solving linear ODEs by converting them into simpler algebraic forms. Any questions before we move on?

Applying the Laplace Transform

Unlock Audio Lesson

0:00
Teacher
Teacher

Let's look at a specific example. Consider the second-order linear ODE: $$y'' + 3y' + 2y = e^{-t}, \quad y(0) = 0, \quad y'(0) = 0$$.

Student 4
Student 4

What is the first step in solving this?

Teacher
Teacher

Great question! The first step is to apply the Laplace Transform to both sides. So we would write: $$L\{y''\} + 3L\{y'\} + 2L\{y\} = L\{e^{-t}\}$$.

Student 1
Student 1

And how do those derivatives transform?

Teacher
Teacher

"Using our earlier properties:

Solving for Y(s)

Unlock Audio Lesson

0:00
Teacher
Teacher

"Now that we have the transformed equation, we can solve for $Y(s)$. The equation we arrive at is:

Inverse Laplace Transform

Unlock Audio Lesson

0:00
Teacher
Teacher

"Now that we have our expression for Y(s), we can find y(t) using the inverse Laplace Transform. This step is crucial!

Introduction & Overview

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

Quick Overview

This section discusses the application of the Laplace Transform in solving second-order linear ordinary differential equations (ODEs) with constant coefficients.

Standard

The section outlines the process of applying the Laplace Transform to second-order linear ODEs, demonstrating solution steps through an example. It emphasizes the transformation of differential equations into algebraic equations for easier solving and the importance of inverse transforms to return to the time domain.

Detailed

Laplace Transform in Solving Differential Equations

In this section, we detail the use of the Laplace Transform to tackle second-order linear ordinary differential equations (ODEs) with constant coefficients. We start with the standard form of a second-order linear ODE:

General Form:
$$ rac{d^2y}{dt^2} + b rac{dy}{dt} + cy = f(t), \quad y(0)=y_0, \quad y'(0)=y_1$$
Here, $a$, $b$, and $c$ are constants, while $f(t)$ represents the forcing function defined on the right side of the equation.

By applying the Laplace Transform, the derivatives convert into algebraic forms:

Transformed Equation:
$$a[s^2Y(s) - sy(0) - y'(0)] + b[sY(s) - y(0)] + cY(s) = F(s)$$
Where $Y(s)$ is the Laplace Transform of $y(t)$ and $F(s)$ is the transform of $f(t)$.

Following these transformations allows us to algebraically solve for $Y(s)$, which can then be further manipulated using inverse transform techniques to find the function $y(t)$.

Example

Take the specific ODE:
$$y'' + 3y' + 2y = e^{-t}, \quad y(0) = 0, \quad y'(0) = 0$$
By following the outlined steps:
1. Apply the Laplace Transform to both sides.
2. Solve the algebraic equation for $Y(s)$.
3. Use partial fractions to simplify.
4. Finally, apply the inverse Laplace Transform to retrieve $y(t)$.
This process effectively uses the Laplace Transform to allow a straightforward solution to differential equations that might otherwise be challenging to solve directly.

Youtube Videos

Laplace Transform to Solve Differential Equations
Laplace Transform to Solve Differential Equations
Application of Laplace Transformation in Differential equations
Application of Laplace Transformation in Differential equations
Laplace Transform | Solution of Ordinary Differential Equation | Concept & Example by GP Sir
Laplace Transform | Solution of Ordinary Differential Equation | Concept & Example by GP Sir
Engineering Mathematics,Laplace Transform
Engineering Mathematics,Laplace Transform
Intro to the Laplace Transform & Three Examples
Intro to the Laplace Transform & Three Examples
Using Laplace Transforms to solve Differential Equations ***full example***
Using Laplace Transforms to solve Differential Equations ***full example***
Sequence and Series | Infinite  Series | Convergnt & Divergent Part -1
Sequence and Series | Infinite Series | Convergnt & Divergent Part -1
Question#4 - Laplace Transform - Application to Ordinary Differential Equation.
Question#4 - Laplace Transform - Application to Ordinary Differential Equation.
LAPLACE TRANSFORMS  ■ SOLUTION  OF ORDINARY DIFFERENTIAL EQUATIONS PART 8●FOR DEGREE; ENGINEERING..
LAPLACE TRANSFORMS ■ SOLUTION OF ORDINARY DIFFERENTIAL EQUATIONS PART 8●FOR DEGREE; ENGINEERING..
Laplace Transform: First Order Equation
Laplace Transform: First Order Equation

Audio Book

Dive deep into the subject with an immersive audiobook experience.

Introduction to the Test Equation

Unlock Audio Book

Signup and Enroll to the course for listening the Audio Book

Consider a second-order linear ODE with constant coefficients:

d²y/dt² + b dy/dt + cy = f(t),
where y(0) = y0, y'(0) = y1.

Detailed Explanation

This equation represents a second-order linear ordinary differential equation (ODE) with constant coefficients. The terms represent the second derivative of y with respect to t, the first derivative of y, and the function f(t) which is the input to the system. The constants a, b, and c define the dynamic characteristics of the system, while y(0) and y'(0) are the initial conditions of the function and its first derivative, respectively.

Examples & Analogies

Think of this equation as a model for a car's motion where y(t) is the position of the car over time. The coefficients relate to factors like acceleration (a), friction (b), and potential energy (c) that influence how the car moves, while the initial conditions indicate the car's starting position and speed.

Applying the Laplace Transform

Unlock Audio Book

Signup and Enroll to the course for listening the Audio Book

Apply Laplace Transform:

a[s²Y(s)−sy0−y1] + b[sY(s)−y0] + cY(s) = F(s)

Detailed Explanation

To solve the ODE using the Laplace transform, we take the transformation of each term. The terms involving derivatives transform according to specific properties of the Laplace transform: the second derivative leads to s²Y(s) with the initial conditions factored in. The result is an algebraic equation in the Laplace domain (Y(s)), which can be solved for Y(s). Here, F(s) is the Laplace transform of the input function f(t).

Examples & Analogies

Imagine translating the dynamics of a car into a language that only talks about speed and position without directly mentioning time—this transition to Laplace transform does just that, allowing us to manipulate the relationships in a clearer, often simpler, way.

Solving for Y(s)

Unlock Audio Book

Signup and Enroll to the course for listening the Audio Book

Solve algebraically for Y(s), then find the inverse Laplace transform to obtain y(t).

Detailed Explanation

Once we have expressed the left side as a function of Y(s), we can rearrange the equation to isolate Y(s). This step is typically followed by algebraic manipulations, like factoring, to make the expression simpler. After obtaining Y(s), the next step is to take the inverse Laplace transform, which allows us to revert from the Laplace domain back to the time domain, revealing y(t).

Examples & Analogies

It’s similar to first solving an equation that is in a different system (like Celsius to Fahrenheit) and then converting it back to the system we understand (like reconverting Fahrenheit back to Celsius). We first manipulate it comfortably in the new system (Laplace) before interpreting results back in the original terms (time).

Example Problem for Clarity

Unlock Audio Book

Signup and Enroll to the course for listening the Audio Book

Example
Solve: y′′ + 3y′ + 2y = e^−t, y(0) = 0, y′(0) = 0
Step 1: Take Laplace on both sides:

1/(s² + 3s + 2) = (s + 1)/(s + 1)
Step 2: Factor and solve:

Y(s) = 1/[(s + 1)(s + 1)(s + 2)]
Apply partial fractions, then take inverse Laplace to get y(t).

Detailed Explanation

This example illustrates the procedure using a specific second-order linear ODE. After taking the Laplace transform of each term, we obtain a rational function in Y(s). The next step is to factor this expression appropriately and use partial fraction decomposition to make taking the inverse transform feasible. Finally, applying the inverse Laplace transform gives the original function in time.

Examples & Analogies

Think of it as assembling a complex LEGO structure. First, you sort out the pieces (Laplace transform), then you figure out how to fit them together in a smart way (solving the equation), and finally, you step back to see the whole completed structure (inverse Laplace transform). This breakdown makes it easier to understand how each individual part connects to create the whole.

Definitions & Key Concepts

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

Key Concepts

  • Laplace Transform: Used to convert differential equations into algebraic form for easier solving.

  • Inverse Laplace Transform: Necessary for retrieving the original function from its transform.

  • Initial Conditions: Key in solving ODEs, helping to define the function's state at a point in time.

Examples & Real-Life Applications

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

Examples

  • Example equation: y'' + 3y' + 2y = e^{-t}, y(0)=0, y'(0)=0.

  • By applying Laplace Transform: s^2Y(s) + 3sY(s) + 2Y(s) = (s + 1)/(s + 1).

Memory Aids

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

🎵 Rhymes Time

  • When solving DEs, give Laplace a chance, turns chaos to calm with a calculating glance.

📖 Fascinating Stories

  • Imagine a student named Ella who struggled with differential equations until she found a magical Transform that turned them into easy algebra. She was then able to solve them in no time, and soon her struggle became a breeze.

🧠 Other Memory Gems

  • To remember the steps of Laplace: Transform, Solve, Inverse - 'TSI' for the tidy solve!

🎯 Super Acronyms

SOFT for 'Solve ODEs Fast with Transforms'!

Flash Cards

Review key concepts with flashcards.

Glossary of Terms

Review the Definitions for terms.

  • Term: Laplace Transform

    Definition:

    An integral transform that converts a time-domain function into a complex frequency domain function.

  • Term: Ordinary Differential Equation (ODE)

    Definition:

    An equation involving derivatives of a function of a single variable.

  • Term: Initial Conditions

    Definition:

    The conditions at the start of the observation (e.g., values of a function and its derivatives at t=0).

  • Term: Inverse Laplace Transform

    Definition:

    The operation that reverses the Laplace Transform, recovering the original time-domain function.

  • Term: Algebraic Form

    Definition:

    A representation of an equation without derivatives, usually easier to solve.