The wave equation is an important second-order linear partial differential equation for the description of waves—as they occur in classical physics—such as mechanical waves (e.g. water waves, sound waves and seismic waves) or light waves. It arises in fields like acoustics, electromagnetics, and fluid dynamics. Due to the fact that the second order wave equation describes the superposition of an incoming and outgoing wave (i.e. rather a standing wave field) it is also called "Two-way wave equation" (in contrast, the 1st order One-way wave equation describes a single wave with predefined wave propagation direction and is much easier to solve due to the 1st order derivatives).
Historically, the problem of a vibrating string such as that of a musical instrument was studied by Jean le Rond d'Alembert, Leonhard Euler, Daniel Bernoulli, and Joseph-Louis Lagrange. In 1746, d’Alembert discovered the one-dimensional wave equation, and within ten years Euler discovered the three-dimensional wave equation.
Homework Statement
Consider the second order wave equation
u_{tt} = 4u_{xx}
There are initial and boundary conditions attached, but I'm less concerned with those for the moment. I think I can figure those out if I can figure out where to get started.
Rewrite this as a system of first order...
Homework Statement
If a system satisfies the equation \nu^2 {\partial^2 \psi\over \partial x^2}={\partial^2 \psi\over \partial t^2}+a{\partial \psi\over \partial t}-b\sin\left({\pi x \over L}\right)\cos\left({\pi \nu t\over L}\right)
subjected to conditions: \psi(0,t)=\psi(L,t)={\partial...
Homework Statement
You know how if you flick one end of a garden hose you can watch the wave travel down, and then back to you? I wrote this MATLAB code to solve the associated PDE via the Fourier method and the resulting animation looks good for a few time steps, but then the solution...
D'Alembert's solution to the wave equation is
u(x,t) = \frac{1}{2}(\phi(x+ct) + \phi(x-ct)) + \frac{1}{2c}\int_{x-ct}^{x+ct} \psi(\xi)d\xi where \phi(x) = u(x,0) and \psi(x) = u_t (x,0). I'm trying to understand this intuitively. The first term I get: a function like f = 0 (x/=0), = a (x=0)...
[b]1.
For the 1-D wave equation, the d’Alembert solution is u(t, x) = f (x + ct) + g(x − ct) where f , g are each a function of 1 variable.
Suppose c = 1 and we know f (x) = x^2 and g(x) = cos 2x for x > 0.
Find u(t, x) for al l t, x ≥ 0 if you are also given the BC: u ≡ 1 at x = 0...
Homework Statement
Consider an isotropic medium with constant conductivity \sigma. There is no free charge present, that is, \rho = 0.
a)What are the appropriate Maxwell equations for this medium?
b)Derive the damped wave equation for the electric field in the medium. Assume Ohm's...
Homework Statement
Write down an equation to describre a wave \psi(x,t) with all of the following properties
a) It is traveling in the negative x direction
b) It has a phase velocity of 2000ms-1
c) It has a frequency of 100kHz
d)It has an amplitude of 3 units
e) \psi(0,0)= 2 units...
Hi there. I was trying to understand this deduction of the one dimensional wave equation developed at the beggining of the book A first course in partial differential equations of H.F. Weinberger.
You can see it right here...
This question is also posted at http://www.mathhelpforum.com/math-help/f59/use-fourier-transform-solve-pde-damped-wave-equation-188173.html
Use Fourier transforms to solve the PDE
\displaystyle \frac{\partial^2 \phi}{\partial t^2} + \beta \frac{\partial \phi}{\partial t} = c^2...
Consider a string of length 5 which is fixed at its ends at x = 0 and x = 5. The speed of waves along the string is v = 2 and the displacement of points on a string is defined by the function f(x,t). At the initial time the string is pulled into the shape of a triangle, defined by
f(x,0) =...
(Note: although arising in QM, this is essentially a calculus question)
Ѱ (x) = A sin (n╥x/a)
1 = ∫ l Ѱ (x) l^2 dx with limits of integration a to 0
1 = ∫ A^2 sin^2 (n╥x/a) dx with limits of integration a to 0
Indefinite integral ∫ sin^2 x dx = x/2 - sin2x/4
I know this integral...
I have just completed Atomic Structure from my textbook. In that a Schrodinger Wave Equation is mentioned and after that it is written that it is not in the scope of this book to solve this equation. I want to know what is so hard in the schrodinger wave equation that it is not of my level?
Homework Statement
The wave equation is
\nabla^2 \mathbf{A}(\mathbf{r},t) = \frac{1}{c^2} \frac{\partial^2 \mathbf{A}(\mathbf{r},t)}{\partial t^2}
I want to get a solution for the vector potential A.
Homework Equations
we can use the Fourier transformation...
Homework Statement
As I know wave equation has d^2/dt^2,but Schrodinger's equation has only d/dt
(Time-dependent).
Why these eq has different thing(d/dt, d^2/dt^2)?
I assume if Schrodinger's equation has d^2/dt^2(not d/dt),
eigenfunction of Schrodinger's equation is not stable along with...
in electromagnetic books, we see by the aid of vector calculus, we can reach to wave equation from Maxwell 's equations.
is it possible to reach to Maxwell 's equations from wave equations?
in the other word, in electromagnetic books we get Maxwell 's equations as phenomenological...
Homework Statement
Well, I'm not sure if this is a correct subforum to post my problem, but to me it does seem to me as an academic problem. One I can not solve, apparently.
Well, anyway. I'm solving the 1+1 radial wave equation using finite difference. I shifted my grid, so that the origin...
Hello everyone and greetings from my internship!
It's weekend and I'm struggling with my numerical solution of a 1+1 wave equation.
Now, since I'm eventually going to simulate a black hole ( :D ) I need a one-side open grid - using advection equation as my boundary condition on the end of my...
Homework Statement
Show that the electromagnetic wave equation
\frac{\partial^{2}\phi}{\partial x^{2}} +
\frac{\partial^{2}\phi}{\partial y^{2}} +
\frac{\partial^{2}\phi}{\partial z^{2}} -
\frac{1}{c^2}\frac{\partial^{2} \phi}{\partial t^2}
is invariant under a Lorentz transformation...
Hello,
My question is about method of characteristics used in solving wave equation. I've found a book on dynamics of structures, and what I cannot understand is a part when it is talked about method of characteristic. Can somebody try to read the shoert article attached below and see if...
Hi,
I want to solve the following wave equation:
u_{tt} - c^2 u_{xx} = f(x,t)u
What is the best way to do it? I don't think I can use Duhamel's principle since I have a u in the forcing.
Doing a change of variables of the form
w=x+ct, v=x-ct
Seems to make things worse.
Any ideas...
Homework Statement
(A)
[PLAIN]http://remote.physik.tu-berlin.de/farm/uploads/pics/Gekoppeltes_Pendel_01.png
What happens when you swing pendulum P1?
(B)
How does the position of the spring affect the outcome?
(C)
If the length of the string of one pendulum was longer than the...
For a traveling wave
u(x,t) = u(x-ct)
How is the relation below hold?
u_{x}u_{xt}=-u_tu_{xx}
I don't understand why there is (-) sign .
Thanks in advance !
PS.
Here is the URL of the book I am having trouble with
https://www.amazon.com/dp/0198528523/?tag=pfamazon01-20...
Wave Equation (urgent)
Sounds waves in a pipe of varying cross-section are described by the wave equation
v2 d/dx .(1/A.dAu/dx) = d2u /dt2
Where A = 0.2 +0.3x simplify the equation
My attempt at a solution
Sub in A:
v2 d/dx ( 1/(0.2+0.3x) . d(0.2+0.3x)u/dx) =d2u/dt2
Not to...
This is the problem, it says to solve the solution to the vibrating string problem.
\frac{\partial^2 u}{\partial t^2}=\frac{\partial^2 u}{\partial x^2}
u(0,t)=u(1,t)=0,t>0
u(x,0)=x(1-x),0<x<1
\frac{\partial u}{\partial t}(x,0)=sin(7\pi x),0<x<1
The solution form I obtained (without showing my...
For a real stretched string, the wave equation is
(partial deriv)^2 (u)/partial deriv t^2 = (T/mu) (partial deriv)^2 (u)/partial deriv x^2 - B/mu(y)
where T is the tension in the string, mu is its mass per unit length and B is its "spring constant".
Show that the wave given by u =...
Hello everybody! I have a really silly question concerning wave equation: consider the problem
\left\{
\begin{matrix}
u_{tt} &=& u_{xx} & x \in \mathbb{R}\\
u(x,0) &=& 0 & \\
u_t(x,0) &=& x(1-x)\chi_{\left[0,1\right]}(x)&
\end{matrix}
\right.
the solution is given by d'Alembert's...
http://www.math.ubc.ca/~feldman/apps/wave.pdf is the link from where I understood how to derive the wave equation. But why is theta assumed to be small? As I understand it, theta is the angle that the string segement we're considering makes with the horizontal. Even a simple sine wave seems to...
Homework Statement
Find the solution u, via the Fourier sine/cosine transform, given:
u_{tt}-c^{2}u_{xx}=0
IC: u(x,0) = u_{t}(x,0)=0
BC: u(x,t) bounded as x\rightarrow \infty , u_{x}(0,t) = g(t)
2. The attempt at a solution
Taking the Fourier transform of the PDE, IC and BC...
Hello!
When considering the acoustics wave equation
\frac{\partial^{2}P}{\partial t^{2}} = c^{2} \nabla^{2} P
I don't really understand why you can say that the applicability of this equation varies for different sound pressure levels. I don't see why this shouldn't hold for all...
Hello.
If I have this equation:
And this general solution:
Would it then be wrong to write the above solution with only positive values of n? In my textbook they often write the result from a superposition with only positive values of n, becasue the negative values of n already...
Homework Statement
Consider the following system of equations: \frac{\partial \vec H}{\partial t} -i \vec \nabla \times \vec H =0 where \vec H is a vector field.
1)Show that \vec Y =\partial _t \vec H satisfies the wave equation.
2)Demonstrate that if \vec \nabla \cdot \vec H=0 initially...
Hi,
I want to solve the forced wave equation
u_{tt}-c^2u_{xx} = f''(x)g(t)
(primes denote derivatives wrt x). The forcing I am interested in is
f(x,t)= e^{-t/T} (\alpha_o+\alpha_1 Tanh(-\frac{(x-x_o)}{L}) .
I also am imposing causality, i.e. u =0 for t<0 .
In the case...
I'm doing a project on a vibrating guitar string and I have completed all the simulation and experimental work, but I do not fully understand the theory behind it. I need to derive the 1 dimensional case of the wave equation, as the 1 dimensional case is considered to be the most convenient...
If I understood well my professor, he showed that "playing" mathematically with Maxwell's equation \frac{\partial \vec E}{\partial t} = c \vec \nabla \times \vec B can lead to the result that \frac{\partial \vec E}{\partial t} satisfies the wave equation (only in vacuum).
So what does this...
Homework Statement
Solve the IVP for the wave equation:
Utt-Uxx=0 for t>0
U=0 for t=0
Ut=[dirac(x+1)-dirac(x-1)] for t=0
2. The attempt at a solution
By D' Almbert's solution:
1/2 integral [dirac(x+1)-dirac(x-1)] dx from (x-t) to (x+t)
I apologize for not using Latex- my...
In solving the driven oscillator without damping, I need to solve the integral
{ exp[-iw(t-t')] / (w)^2 - (w_0)^2 } .dw
where w_0 is the natural frequency.
I know the poles lie in the lower half plane, yet I cannot see why. If (t - t') < 0, the integral is zero. I am not exactly sure...
So, I do not think I did this properly, but if f(-x)=-f(x), then u(-x,0)=-u(x,0), and if g(-x)=-g(x), then ut(-x,0)=-ut(x,0).
According to D`Alambert`s formula,
u(x,t)=[f(x+t)+f(x-t)]/2 + 0.5∫g(s)ds (from x-t to x+t)
so, u(0,t)=[f(t)+f(-t)]/2 + 0.5∫g(s)ds (from -t to t)
f is odd, and so is...
Homework Statement
Solve the boundary value problem (1)-(3) with a=b=1, c=1/Π
f(x)=sin(3 \pi x) sin(\pi y),g(x)=0
(1)\frac{\partial^{2}u}{\partial t^{2}}=c^{2}\left(\frac{\partial^{2}u}{\partial x^{2}}+\frac{\partial^{2}u}{\partial y^{2}}\right) 0 < x < a, 0< y <b, t > 0
(2)...
Homework Statement
I have a homework problem that says that any function of the below form is a solution to the homogeneous wave equation.
Any function of this form is a solution to the following equation:
I would be able to solve it if the function was defined, but I'm not...
Homework Statement
Derive the general nontrivial relation between \phi and \psi which will produce a solution to u_{tt}-u_{xx}=0 in the xt-plane satisfying
u(x,0)=\Phi(x) and u_t(x,0)=\Psi(x) for -\infty\leq x \leq \infty
and such that u consists solely of a wave traveling to the left along...
Homework Statement
Consider the partial differential equation
u_{xx}-3u_{xt}-4u_{tt}=0
(a) Find the general solution of the partial differential equation in the xt-plane, if possible.
(b) Find the solution of the partial differential equation that satisfies
u(x,0)=x^3 and...
Homework Statement
"Solve for t > 0 the one-dimensional wave equation
\frac{\partial^2 u}{\partial t^2} = c^2 \frac{\partial^2 u}{\partial x^2}
with x > 0, with the use of Fourier transformation.
The boundary condition in x = 0 is u(0,t) = 0.
Assume that the initial values u(x,0) and...
Hi all
I was wondering if I could solve the schrodinger's equation to see the limiting velocity for a proton to tunnel through the coulomb gap in order for the first equation in the fusion reaction to occur
Thanks a lot
inhomogeneous Klein-Gordon equation solution?
Homework Statement
Psi_xx - Psi_tt - 4Psi = exp(exp(3it))*dirac_delta(x)
DE valid for all x,t (no boundary conditions specified).
Homework Equations
Solve for Psi. If the DE is singular, then nontrivial solutions are okay.
The Attempt at a...
On my notes, the lecturer left out some of the formulae as blanks which we were supposed to fill in as we went a long but I'm missing a few of them. The 1st one is:
[PLAIN]http://img213.imageshack.us/img213/6627/screenshotdh.png
I'm stuck here, I can't figure out what equation he's...
Infinite string at rest for t<0, has instantaneous transverse blow at t=0 which gives initial velocity of V \delta ( x - x_{0} ) for a constant V. Derive the position of string for later time.
I thought that this would be y_{tt} = c^{2} y_{xx} with y_{t} (x, 0) = V \delta ( x - x_{0} ) ...
For plane wave travel in +ve z direction in a charge free medium, the wave equation is:
\frac{\partial^2 \widetilde{E}}{\partial z^2} -\gamma^2 \widetilde E = 0
Where \gamma^2 = - k_c^2 ,\;\; k_c= \omega \sqrt {\mu \epsilon_c} \hbox { and } \epsilon_c = \epsilon_0 \epsilon_r...
I've attached the problem sheet with the given bottom line numerical answers. I'm struggling with question 3 part d and the solution sheet doesn't include the answer to this part of the question. I've completed the previous parts to question 3 already.
Can someone please guide me through...
Homework Statement
Two vibrating sources emit waves in the same elastic medium. The first source has a frequency of 25 Hz, while the 2nd source's frequency is 75 Hz. Waves from the first source have a wavelength of 6.0 m. They reflect from a barrier back into the original medium, with an...