Worked Example - 11.1.7 | 11. One-Dimensional Wave Equation | Mathematics - iii (Differential Calculus) - Vol 2
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Interactive Audio Lesson

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

Introduction to the Wave Equation

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0:00
Teacher
Teacher

Let's start with the basics. What is the one-dimensional wave equation?

Student 1
Student 1

Is it the equation that describes how waves propagate through a medium?

Teacher
Teacher

Exactly! The wave equation models the movement of waves, such as sound or water waves, along one dimension. Can anyone tell me the standard form of this equation?

Student 2
Student 2

I think it goes like this: \( \frac{\partial^2 u}{\partial t^2} = c^2 \frac{\partial^2 u}{\partial x^2} \)!

Teacher
Teacher

Great! Here, \(u(x,t)\) represents displacement, and \(c\) is the wave speed. Remember this equation as it is foundational in understanding wave behavior.

Setting the Problem

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Teacher
Teacher

Now, let’s take a look at our specific problem. We have the wave equation: \( \frac{\partial^2 u}{\partial t^2} = 4 \frac{\partial^2 u}{\partial x^2} \). What boundary conditions do we have?

Student 3
Student 3

We have \(u(0,t) = 0\) and \(u(\pi,t) = 0\).

Teacher
Teacher

Right! These fixed boundary conditions mean the ends of our string do not move. And what about the initial conditions?

Student 4
Student 4

The initial displacement is \(u(x,0) = \sin(x)\), and the initial velocity is \(\frac{\partial u}{\partial t}(x,0) = 0\).

Teacher
Teacher

Perfect! We will use these to find our solution.

Applying Separation of Variables

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Teacher
Teacher

To solve this using separation of variables, we assume a solution of the form \(u(x,t) = X(x)T(t)\). Can anyone derive this relationship?

Student 1
Student 1

We break the equation into two parts: one depending on \(x\) and the other on \(t\).

Teacher
Teacher

Exactly! By substituting back into our wave equation, we can separate the variables. Now, given that the initial displacement is \(\sin(x)\), how does this help us express the solution?

Student 2
Student 2

It tells us that the solution will involve the sine function for the spatial part!

Teacher
Teacher

Great! So what would our solution be?

Student 3
Student 3

I think it would be \(u(x,t) = \cos(2t)\sin(x)\)!

Teacher
Teacher

Exactly right! This shows the wave behavior with respect to time and space.

Concluding the Example

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Teacher
Teacher

To summarize, we covered how we set the boundary and initial conditions for our wave equation problem. We used separation of variables to arrive at our solution, which demonstrates how waves propagate in the string.

Student 4
Student 4

So, we basically applied the principles from earlier sections and now we see how they connect to real wave scenarios!

Teacher
Teacher

Precisely! Understanding this worked example helps solidify our grasp on solving wave equations with real-world applications.

Introduction & Overview

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

Quick Overview

This section presents a worked example of solving the one-dimensional wave equation with specific initial and boundary conditions.

Standard

In this section, we solve the wave equation using separation of variables, focusing on fixed boundary conditions and initial displacement. The method leads to the solution for a vibrating string modeled by the sine function.

Detailed

Worked Example of the One-Dimensional Wave Equation

In this section, we explore a worked example of the one-dimensional wave equation:

$$ \frac{\partial^2 u}{\partial t^2} = 4 \frac{\partial^2 u}{\partial x^2} $$

for the domain $0 < x < \pi$ with given boundary conditions:
- $u(0,t) = 0$
- $u(\pi,t) = 0$
- Initial displacement: $u(x,0) = \sin(x)$
- Initial velocity: $\frac{\partial u}{\partial t}(x,0) = 0$

Solution:

To solve this wave equation, we employ the method of separation of variables. We look for solutions of the form $u(x,t) = X(x)T(t)$. Given that the initial displacement is $\sin(x)$, we deduce:

$$ u(x,t) = \cos(2t)\sin(x) $$

This demonstrates how the wave propagates through the medium while adhering to the defined boundary and initial conditions.

Key Takeaways:

  • The wave equation models wave propagation in various media.
  • Separation of variables is a powerful technique for finding specific solutions given boundary and initial conditions.

Youtube Videos

But what is a partial differential equation?  | DE2
But what is a partial differential equation? | DE2

Audio Book

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Problem Statement

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Problem: Solve the wave equation
βˆ‚Β²π‘’/βˆ‚π‘‘Β² = 4, for 0 < π‘₯ < πœ‹, with:
- 𝑒(0,𝑑) = 0, 𝑒(πœ‹,𝑑) = 0
- βˆ‚π‘’/βˆ‚π‘‘ (π‘₯,0) = 0
- 𝑒(π‘₯,0) = sin(π‘₯)

Detailed Explanation

In this example, we are tasked with solving a specific wave equation subject to fixed boundary conditions and an initial displacement. The wave equation given is a second-order partial differential equation that describes how waves propagate over time. The boundary conditions state that at position 0 and Ο€, the wave displacement is fixed at zero. Additionally, the initial conditions specify that the wave’s initial velocity at any point in time is zero and its initial displacement is represented by the function sin(x).

Examples & Analogies

Imagine plucking a guitar string. The ends of the string (0 and C0 in this case) cannot move, just as the fixed boundary conditions ensure the displacement there is zero. The initial shape of the string (the initial displacement) reflects a sine wave, similar to how the vibrating string creates sound waves.

Separation of Variables

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Solution: We use separation of variables:

Since initial displacement is sin(π‘₯), we find:
𝑒(π‘₯,𝑑) = cos(2𝑑)sin(π‘₯)

Detailed Explanation

To solve the wave equation, we apply the method of separation of variables. This technique involves rearranging the wave equation into a form where the variables can be separated, allowing us to handle the spatial and temporal components independently. In this case, we recognize that the initial displacement being sin(x) informs our solution's spatial component. The time component, which represents oscillations, is captured by cos(2t) because it corresponds to the wave’s frequency. Combining these leads to the solution u(x,t) = cos(2t)sin(x), which shows how the wave changes over time in a fixed-length medium.

Examples & Analogies

Think of a swing on a playground. When you push it, it oscillates back and forth (that’s the cos part), while the specific height it reaches at any point in time is influenced by how hard you initially pushed it (that’s the sin part). Together, they explain the motion of the swing just like they describe the wave in our example.

Summary of the Worked Example

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Summary:
- The one-dimensional wave equation models vibrations and wave propagation in strings and similar media.
- The equation is derived from Newton’s laws and string tension considerations.
- D’Alembert’s solution handles infinite domains, while separation of variables is used for bounded domains.
- Boundary and initial conditions are crucial for determining specific solutions.
- The general solution for fixed ends involves Fourier sine series expansions.

Detailed Explanation

In summary, we've solved a wave equation by applying the separation of variables technique, which is particularly effective for problems with fixed boundaries. The results illustrate the fundamental principles of wave motion and how specific initial and boundary conditions dictate the wave's behavior. Recognizing the important role of these conditions helps validate the method we used and illustrates the broader utility of the wave equation in modeling real-world scenarios.

Examples & Analogies

Consider a drum skin. When struck, it vibrates to create sound waves. The wave propagation can be thought of in terms of our equation where the way the drum is initially struck (initial conditions) and the edges of the drum (boundary conditions) significantly affect the sound produced. This connection shows the importance of understanding the underlying equations and conditions to predict and analyze various physical phenomena.

Definitions & Key Concepts

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

Key Concepts

  • Wave Equation: A partial differential equation describing wave propagation.

  • Boundary Conditions: Fixed constraints at the ends of the medium.

  • Initial Conditions: Values that define the state of the wave at time t=0.

  • Separation of Variables: A technique used to simplify partial differential equations.

Examples & Real-Life Applications

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

Examples

  • Example of the wave equation for a vibrating string fixed at both ends.

  • Solution indicating that the wave oscillates over time described by trigonometric functions.

Memory Aids

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

🎡 Rhymes Time

  • In waves so bright, equations take flight, 'Round fixed ends, they dance right.

πŸ“– Fascinating Stories

  • Imagine a string held at both ends, vibrating to the tune of wave equations, echoing through times, gaining speed and form.

🧠 Other Memory Gems

  • WAVE: When Analyzing Various Equations, remember the wave behavior at endpoints.

🎯 Super Acronyms

B.I.W. for Boundary, Initial, and Wave equation – key terms in solving wave problems.

Flash Cards

Review key concepts with flashcards.

Glossary of Terms

Review the Definitions for terms.

  • Term: Wave Equation

    Definition:

    A second-order linear partial differential equation that describes wave propagation in a medium.

  • Term: Initial Conditions

    Definition:

    Conditions that specify the state of the system at the beginning of observation.

  • Term: Boundary Conditions

    Definition:

    Constraints that are applied at the boundaries of the domain in a differential equation.

  • Term: Separation of Variables

    Definition:

    A mathematical method used to solve partial differential equations by separating variables.