Solving the Vertical Plane Pendulum: Energy Levels & Corrections

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SUMMARY

The discussion focuses on solving the energy levels of a vertical plane pendulum system, where a mass m is attached to a massless rod of length l. The participants explore classical mechanics and quantum mechanics, specifically using the Schrödinger equation to derive energy levels and corrections for small angles. Key equations include the Hamiltonian H = T + V, with potential energy V approximated as V = mgl(1 - cos(θ)) and kinetic energy T = p²/2m. The lowest-order correction to the ground state energy is derived using Taylor series expansions, resulting in E'₀ = 3/4 α⁴(-1/24 mgl/l³).

PREREQUISITES
  • Understanding of classical mechanics, specifically pendulum motion.
  • Familiarity with quantum mechanics and the Schrödinger equation.
  • Knowledge of Taylor series expansions and their applications in physics.
  • Basic concepts of Hamiltonian mechanics and energy conservation.
NEXT STEPS
  • Study the derivation of the Schrödinger equation for simple harmonic oscillators.
  • Learn about Taylor series and their applications in approximating functions in physics.
  • Explore the concept of Hamiltonian mechanics in greater depth.
  • Investigate the implications of small-angle approximations in pendulum dynamics.
USEFUL FOR

Students and professionals in physics, particularly those focusing on classical mechanics and quantum mechanics, as well as anyone interested in solving complex systems involving energy levels and corrections.

eman2009
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Homework Statement


a mass m is attached by a massless rod of length l to a pivot , which allows swing freely in a vertical plane under the influence of gravity .let the anglethita betweenthe rod the vertical .
find the energy levels of the system?
find the lowest -order correction to the ground state energy with small angle?

Homework Equations





The Attempt at a Solution


if i can solve it classically first and then find the energy from schrodenger eqn , but I'm not sure if the hamiltonain work in this case?
 
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hmmm... have a look what the simplified potential would look like (ie for small angles) should hopefully give you a hint
 
v=-mg cos thita
T= p^2/2m
H=T+V
put in schrodenger eqn solve for E then find the energy level...?
and for small angle thita =0 is it like this
 
like what? try expanding cos(theta) for small theta, the potential should look familiar
 
V=mgl
cos thita=1 for small thita
howabout the boundary condition ... if the angle is small is it
FI =FI(thita+2bi)
or
FI(0)=0
FI the wave function
 
i'm not sure what you last post means

try writing what the force - F = -dV/dx,

do you know taylor series? if so you could expand both the potential (cos term) & the force (sin) for small theta

i think it will look soemthing like
F ~ -k.x

similarly
V ~ k.x^2

look familiar? looking simply harmonic to me...
 
i think i got the answer is it totally differnet
look...v=mgl(1-costhita)
H=1/2 ml^2thita'^2+1/2 mglthita^2
and E=(n-1/2)hw but i don't know from where get the E?
the lowest correction is H'=v-1/2 ml thita^2=1/24mglthita^4 , how ?
E'0=3/4 alpha^4(-1/24mgl/l^3)...how?
 
try the taylor series expansion and show some working
 
for what i use tylar expansion can you clear it please
 
  • #10
taylor expansions

cos(t) ~1 + t^2/2 +o(t^4)
sin(t) ~ t + o(t^3)
 

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