Hamiltonian and Conjugate Momenta in a Two-Dimensional Potential

[stunner5000pt]

Particle of mass m moves in two dimensionas un der the influence of a potential V(x,y) = kxy where K > 0 (not a cetnral potential)

a) Determine the momenta conjugate to the coordiante x,y of this system and Hamiltonian punction of this system (in terms of the coordiante and conjugate momenta). Explian whether the Hamilton is a constant of motion

H = \frac{1}{2m} (p_{x}^2 + p_{y}^2} + kxy

wouldnt hte momenta simply be p_{q} = m\dot{q} where q is a coordinate?
well the Hamitlon doesn't dependa on timte epxlicitly so it is constnat of motion

so far so good?

thank you for ANY help

 

[topsquark]

Particle of mass m moves in two dimensionas un der the influence of a potential V(x,y) = kxy where K > 0 (not a cetnral potential)

a) Determine the momenta conjugate to the coordiante x,y of this system and Hamiltonian punction of this system (in terms of the coordiante and conjugate momenta). Explian whether the Hamilton is a constant of motion

H = \frac{1}{2m} (p_{x}^2 + p_{y}^2} + kxy

wouldnt hte momenta simply be p_{q} = m\dot{q} where q is a coordinate?
well the Hamitlon doesn't dependa on timte epxlicitly so it is constnat of motion

so far so good?

thank you for ANY help

q is a generalized coordinate and so will not always have units of distance. So p is not automatically m(dq/dt). In general:
\dot p_j=-\frac{\partial H}{\partial q_j}.

Yes, if H has no explicit time dependence, then H is a constant of the motion.

-Dan

 

[stunner5000pt]

q is a generalized coordinate and so will not always have units of distance. So p is not automatically m(dq/dt). In general:
\dot p_j=-\frac{\partial H}{\partial q_j}.

Yes, if H has no explicit time dependence, then H is a constant of the motion.

-Dan

so do i use the lagrangian which is L = T-V to get the Hamiltonian

doing that yielded
H = \frac{1}{2} m \dot{x}^2 - \frac{1}{2} m \dot{y}^2 + kxy
if i did it for x and x dot
the signs of the first tow terms were switched when i did it for y

 

[pmb_phy]

Particle of mass m moves in two dimensionas un der the influence of a potential V(x,y) = kxy where K > 0 (not a cetnral potential)

a) Determine the momenta conjugate to the coordiante x,y of this system and Hamiltonian punction of this system (in terms of the coordiante and conjugate momenta). Explian whether the Hamilton is a constant of motion

H = \frac{1}{2m} (p_{x}^2 + p_{y}^2} + kxy

wouldnt hte momenta simply be p_{q} = m\dot{q} where q is a coordinate?
well the Hamitlon doesn't dependa on timte epxlicitly so it is constnat of motion

so far so good?

thank you for ANY help

Are you looking for the mechanical linear momentum or the canonical momentum? If the later then obtain the Lagrangian for this system from the Hamiltonian. Express all varibles in terms of generalized velocities. From this you can take the partial derivative of the Lagrangian with respect to the generalized velocity conjugate to the appropriate coordinate.

That should give you enough to start. It may be a bit difficult for you to do this transformation (Which I believe is called an inverse Legendre transformation), Good luck.

Pete

 

[stunner5000pt]

i am loking for hte canonical momentum (i think) but i don't believe we have touched on inverse legendre tranformations

however
L = \frac{1}{2} m\dot{r}^2 - kxy
where r(t) = (x(t),y(t))

right?
so do i do
H = \dot{r} \frac{\partial L}{\partial \dot{r}} - L??

but what about hte x and y?

 

[pmb_phy]

i am loking for hte canonical momentum (i think) ..

That is correct. The hint to that is that they asked for the momentum conjugate to x and y. That means that canonical momentum.

..but i don't believe we have touched on inverse legendre tranformations

Its a tricky business in general but in this case its a snap. You have the kinetic energy and the potential energy. You must have the Lagrangian expressed in terms of v_x and v_y. The Lagrangian is

L = \frac{1}{2m}\dot{x}^2 + \dot{y}^2 - kxy

Now use the definition of conjugate momenta

p_x = \frac{\partial L}{\partial \dot{x}}

p_y = \frac{\partial L}{\partial \dot{y}}

Good luck and let me know if you have more quetions. It'd be good for you to look up the term "Legendre transformation" in a classical mechanics text such as Goldstein's.

Pete