14.5 - Final Form of D'Alembert’s Solution (with initial conditions)
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Introduction to D'Alembert's Solution
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Today, we’ll explore D'Alembert's solution to the one-dimensional wave equation. What do you recall about this equation?
It describes how waves, like sound or light, travel in a medium.
Exactly! The equation is \( \partial^2 u / \partial t^2 = c^2 \partial^2 u / \partial x^2 \). D'Alembert's solution gives us wave behavior in a specific form. Can anyone tell me what that form looks like?
Isn’t it \( u(x, t) = f(x + ct) + g(x - ct) \)?
Correct! This representation shows how shapes of waves travel without distortion. We’ll now dive deeper into applying initial conditions to this solution.
Applying Initial Conditions
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Great! Now, let's think about what happens when we have initial conditions. How do we define them in the context of wave equations?
We define initial displacement \( \phi(x) \) and initial velocity \( \psi(x) \).
"Correct! By applying these initial conditions, we can express D'Alembert’s solution more completely. It's given by:
Physical Interpretation of the Solution
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So far, we have seen the mathematical formulation. How do the terms in D'Alembert’s solution relate to physical wave behavior?
The terms show how the wave moves based on initial conditions, right?
Exactly! The displacement terms provide insight into how the wave propagates as per the initial settings. The integral shows how velocity dynamically influences the wave shape.
Can we use this to predict wave behavior?
Definitely! Understanding these aspects enables us to solve diverse wave problems accurately. Let's summarize what we learned.
D'Alembert's Example Problem
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Let’s apply our knowledge to solve a practical wave equation problem. We have the wave equation with \( u(x, 0) = ext{sin}(x) \) and \( \partial u / \partial t (x, 0) = 0 \). What steps can we take?
First, we identify \( c = 2 \), then \( \phi(x) = ext{sin}(x) \) and \( \psi(x) = 0 \).
Correct! Now, can you apply D'Alembert’s solution using these conditions?
"Using D'Alembert's formula, we get:
Introduction & Overview
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Quick Overview
Standard
This section elaborates on D'Alembert's solution to the one-dimensional wave equation, detailing how initial conditions can be applied to derive a complete formula for wave motion. It highlights the significance of initial displacement and velocity and their roles in determining the wave behavior over time.
Detailed
In this section, we delve into the final form of D'Alembert’s solution for the one-dimensional wave equation, which is crucial in mathematical physics for describing wave phenomena. The solution is represented as:
\[ u(x, t) = \frac{1}{2} [\phi(x + ct) + \phi(x - ct)] + \frac{1}{2c} \int \psi(s) ds \]
Here, \( \phi(x) \) represents the initial displacement and \( \psi(x) \) the initial velocity of the wave. The first term illustrates the effect of initial displacements propagating in both directions, while the second term accounts for how the initial velocity contributes to the overall wave shape. This comprehensive formula offers insights into the nature of wave propagation, ensuring that the wave maintains its shape while moving through the medium.
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Understanding Each Component of the Formula
Chapter 1 of 2
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Chapter Content
1 1 𝑥+𝑐𝑡
• The first term [𝜙(𝑥+ 𝑐𝑡)+ 𝜙(𝑥− 𝑐𝑡)] represents the initial displacement propagating in both directions.
2 2𝑐
• The second term ∫ 𝜓(𝑠) d𝑠 accounts for the initial velocity of the wave.
2𝑐 𝑥−𝑐𝑡
Together, they describe a wave propagating without distortion along a string.
Detailed Explanation
The formula consists of two essential components. The first term, [𝜙(𝑥+𝑐𝑡)+ 𝜙(𝑥− 𝑐𝑡)], indicates how the shape of the wave from the initial displacement 𝜙 expands in both directions (to the left and right) over time. The speed of propagation is reflected in the factor of 𝑐, which denotes how quickly the wave travels. The second term ∫ 𝜓(𝑠) d𝑠 represents the initial velocity effect, which captures how the wave's motion differs from just being displaced. When both components work together, they show that not only does the wave move (change position), but it also maintains its shape as it travels through the medium, ensuring that the wavefront remains intact.
Examples & Analogies
Consider a long bungee cord stretched out. When you pull on one end and release it (creating an initial displacement), that movement creates waves traveling down the cord in both directions. The first part of the equation models the initial wave that moves outwards. If you were to snap the bungee cord again quickly (this is like giving it an initial velocity), the second part of the formula captures how that quick motion affects the travel of the wave along the rope, again ensuring that the shape of the wave remains consistent as it moves.
Putting It All Together
Chapter 2 of 2
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Chapter Content
• This method is central to wave mechanics, string vibrations, acoustics, and other physical systems.
Detailed Explanation
The D'Alembert solution is not just a mathematical tool; it plays a crucial role in understanding various physical phenomena. By providing a clear framework for analyzing waves, this solution helps in calculating behaviors in musical instruments (like how strings vibrate), in predicting wave propagation in fluids (like water waves), and in designing technologies involving sound (like acoustics in auditoriums). It's a foundational tool in physics and engineering that models how waves behave in different environments.
Examples & Analogies
Think about a guitar string when it is plucked. The vibrations travel as waves through the string and into the air, creating the sound you hear. The D'Alembert solution allows engineers and musicians to predict and manipulate these vibrations to create desired sounds. Similarly, when designing bridges or buildings, understanding how waves travel through materials can inform how structures are built to withstand forces like earthquakes or wind.
Key Concepts
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D'Alembert's Solution: Provides a comprehensive way to express wave propagation involving both initial displacement and initial velocity.
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Wave Propagation: The way waves travel through a medium is described by the solution that distinguishes between initial conditions.
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Linear Superposition: The ability to break down complex waves into simpler left and right moving components.
Examples & Applications
In a practical example, given \( u(x, 0) = ext{sin}(x) \) and \( \partial u / \partial t (x, 0) = 0 \), the full wave solution is derived as \( u(x, t) = ext{sin}(x)\cos(2t) \).
If initial displacement is a pulse represented as \( \phi(x) = e^{-x^2} \) and initial velocity \( \psi(x) = 0 \), we can analyze how this pulse propagates.
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Rhymes
D'Alembert shows the wave's grace,
Stories
Imagine a calm lake disturbed by a thrown pebble. The pebble represents the initial displacement, while the ripples are the waves that form based on the pebble's drop point and speed.
Memory Tools
D.A.W.E: D’Alembert, Apply conditions, Wave propagation, Equation.
Acronyms
WAVE
Wave and velocity effects intertwined.
Flash Cards
Glossary
- D'Alembert's Solution
An analytical solution for the one-dimensional wave equation that demonstrates how waves propagate based on initial conditions.
- Initial Conditions
Values specified to determine the state of a system at the beginning of analysis, specifically initial displacement and velocity in wave equations.
- Wave Equation
A second-order linear partial differential equation that describes wave propagation.
- Displacement
The change in position of the wave as a function of time and space.
- Velocity
The rate of change of displacement; in this context, the initial velocity of a wave.
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