What is the physical interpretation of the Lagrangian condition b2-ac ≠ 0?

humanist rho
Messages
92
Reaction score
0

Homework Statement


A Lagrangian for a particular physical system can be written as,

L^{\prime }=\frac{m}{2}(a\dot{x}^{2}+2b\dot{x}\dot{y}+c\dot{y}^{2})-\frac{K%<br /> }{2}(ax^{2}+2bxy+cy^{2})

where a and b are arbitrary constants but subject to the condition that b2
-ac≠0.What are the equations of motion?Examine particularly two cases a=0=c and b=0,c=a.What is the physical system described by above lagrangian.? What is the significance for the condition b2-ac?

2. The attempt at a solution

I've done the mathematics.But donno the physics!

Equations of motion are,
ma\ddot{x}+mb\dot{y}+Kax+Kby=0

ma\ddot{y}+mb\dot{x}+Kcy+Kbx=0

I think these equations represent coupled 2D harmonic oscillator.(i'm not sure)

when a=c=0,
mb\dot{y}+Kby=0
mb\dot{x}+Kbx=0

when b=0,c=-a,

ma\ddot{x}+Kax=0
ma\ddot{y}+Kay=0

Thanks.
 
Physics news on Phys.org
Hello! In general, the system described by the lagrangian represents two "independent" harmonic oscillators, in a sense I'm going to explain: you can collect the coordinates in a vector \vec{v}=(x,y)^t and the coefficient a,b,c in a matrix M such that M_{11}=a, M_{12}=M_{21}=b, M_{22}=c; the lagrangian takes the following form:

L=\frac{m}{2}\dot{\vec{v}^t}M\dot{\vec{v}}-\frac{K}{2}\vec{v}^t M \vec{v}.

Since M is symmetric, we diagonalize it through an orthogonal matrix O:
M=O^t M^{\text{diag}} O.

We can now define two new coordinates x' and y' that can be incorporated in a vector \vec{v&#039;}=(x&#039;,y&#039;)^t which is equal by definition to

\vec{v&#039;}=O\vec{v}.

In this case the lagrangian has manifestly the form of two decoupled harmonc oscillators (if b^2-ac different from zero).
The significance of b^2-ac different from zero means that the two eigenvalues of M are different from zero and, so there are two modes which oscillate.

As far as I know (and if I don't forget any hypothesis), this is a quite general feature of lagrangian which are at most quadratic in the coordinates. I hope this is right and the answer you need,
Francesco
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top