Industry-relevant training in Business, Technology, and Design to help professionals and graduates upskill for real-world careers.
Fun, engaging games to boost memory, math fluency, typing speed, and English skillsβperfect for learners of all ages.
Listen to a student-teacher conversation explaining the topic in a relatable way.
Signup and Enroll to the course for listening the Audio Lesson
Let's start with the basics. What is the one-dimensional wave equation?
Is it the equation that describes how waves propagate through a medium?
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?
I think it goes like this: \( \frac{\partial^2 u}{\partial t^2} = c^2 \frac{\partial^2 u}{\partial x^2} \)!
Great! Here, \(u(x,t)\) represents displacement, and \(c\) is the wave speed. Remember this equation as it is foundational in understanding wave behavior.
Signup and Enroll to the course for listening the Audio Lesson
Now, letβs 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?
We have \(u(0,t) = 0\) and \(u(\pi,t) = 0\).
Right! These fixed boundary conditions mean the ends of our string do not move. And what about the initial conditions?
The initial displacement is \(u(x,0) = \sin(x)\), and the initial velocity is \(\frac{\partial u}{\partial t}(x,0) = 0\).
Perfect! We will use these to find our solution.
Signup and Enroll to the course for listening the Audio Lesson
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?
We break the equation into two parts: one depending on \(x\) and the other on \(t\).
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?
It tells us that the solution will involve the sine function for the spatial part!
Great! So what would our solution be?
I think it would be \(u(x,t) = \cos(2t)\sin(x)\)!
Exactly right! This shows the wave behavior with respect to time and space.
Signup and Enroll to the course for listening the Audio Lesson
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.
So, we basically applied the principles from earlier sections and now we see how they connect to real wave scenarios!
Precisely! Understanding this worked example helps solidify our grasp on solving wave equations with real-world applications.
Read a summary of the section's main ideas. Choose from Basic, Medium, or Detailed.
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.
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: $\frac{\partial u}{\partial t}(x,0) = 0$
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.
Dive deep into the subject with an immersive audiobook experience.
Signup and Enroll to the course for listening the Audio Book
Problem: Solve the wave equation
βΒ²π’/βπ‘Β² = 4, for 0 < π₯ < π, with:
- π’(0,π‘) = 0, π’(π,π‘) = 0
- βπ’/βπ‘ (π₯,0) = 0
- π’(π₯,0) = sin(π₯)
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 waveβs initial velocity at any point in time is zero and its initial displacement is represented by the function sin(x).
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.
Signup and Enroll to the course for listening the Audio Book
Solution: We use separation of variables:
Since initial displacement is sin(π₯), we find:
π’(π₯,π‘) = cos(2π‘)sin(π₯)
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 waveβs 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.
Think of a swing on a playground. When you push it, it oscillates back and forth (thatβs the cos part), while the specific height it reaches at any point in time is influenced by how hard you initially pushed it (thatβs the sin part). Together, they explain the motion of the swing just like they describe the wave in our example.
Signup and Enroll to the course for listening the Audio Book
Summary:
- The one-dimensional wave equation models vibrations and wave propagation in strings and similar media.
- The equation is derived from Newtonβs laws and string tension considerations.
- DβAlembertβs 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.
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.
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.
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.
See how the concepts apply in real-world scenarios to understand their practical implications.
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.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In waves so bright, equations take flight, 'Round fixed ends, they dance right.
Imagine a string held at both ends, vibrating to the tune of wave equations, echoing through times, gaining speed and form.
WAVE: When Analyzing Various Equations, remember the wave behavior at endpoints.
Review key concepts with flashcards.
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.