When Will the Particle Reach Infinity with Given Initial Values?

In summary, the particle reaches infinity at a time t when the Hamiltonian equation H(p,x)=(1/2)p^2 -(1/2)x^4 is constant, resulting in a first-order differential equation for x(t). The mass is assumed to be 1, and the initial conditions x(0)=1 and p(0)=1 can be used to solve for the value of x at the time t.
  • #1
1670frank
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Homework Statement



At what time does the particle reach infinity given that H(p,x)=(1/2)p^2 -(1/2)x^4. And initial values are x(0)=1 and p(0)=1

Homework Equations

The hamiltonian equations i believe are given by the partial derivatives let d mean partial derivative so x'=dH/dp and p'=-dH/dx

The Attempt at a Solution

well so far i have that x'=p and p'=2x^3 but at this point, I am confused over how to impose the initial values... This is my attempt. By separation of variables, dx/dt=p so (1/p)x=t+ c by integration and now i impose initial value of x(0)=1which gives me c=1/p so i get t=(1/p)x-(1/p) and for dp/dt i got t=(1/2x^3)p - (1/2x^3) . At this point I am very confused what to do next or if I am doing this right in the first place... How can i tell when the particle reaches infinity with two times??
 
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  • #2
1670frank said:

Homework Statement



At what time does the particle reach infinity given that H(p,x)=(1/2)x^2 -(1/2)x^4. And initial values are x(0)=1 and p(0)=1

Homework Equations




The hamiltonian equations i believe are given by the partial derivatives let d mean partial derivative so x'=dH/dp and p'=-dH/dx

The Attempt at a Solution

well so far i have that x'=p and p'=2x^2 but at this point, I am confused over how to impose the initial values... This is my attempt. By separation of variables, dx/dt=p so (1/p)x=t+ c by integration and now i impose initial value of x(0)=1which gives me c=1/p so i get t=(1/p)x-(1/p) and for dp/dt i got t=(1/2x^3)p - (1/2x^3) . At this point I am very confused what to do next or if I am doing this right in the first place... How can i tell when the particle reaches infinity with two times??

You wrote H(p,x)=(1/2)x^2 -(1/2)x^4. Did you mean H(p,x) = (1/2)p^2 - (1/2)x^4?
 
  • #3
Yes thanks for that :)
 
  • #4
1670frank said:
i have that x'=p and p'=2x^2
p' = 2x3?
but at this point, I am confused over how to impose the initial values... This is my attempt. By separation of variables, dx/dt=p so (1/p)x=t+ c
Doesn't look valid to me. Try looking at x''.
 
  • #5
1670frank said:

Homework Statement



At what time does the particle reach infinity given that H(p,x)=(1/2)x^2 -(1/2)x^4. And initial values are x(0)=1 and p(0)=1

Homework Equations




The hamiltonian equations i believe are given by the partial derivatives let d mean partial derivative so x'=dH/dp and p'=-dH/dx

The Attempt at a Solution

well so far i have that x'=p and p'=2x^2 but at this point, I am confused over how to impose the initial values... This is my attempt. By separation of variables, dx/dt=p so (1/p)x=t+ c by integration and now i impose initial value of x(0)=1which gives me c=1/p so i get t=(1/p)x-(1/p) and for dp/dt i got t=(1/2x^3)p - (1/2x^3) . At this point I am very confused what to do next or if I am doing this right in the first place... How can i tell when the particle reaches infinity with two times??

If I were dong this question I would avoid the dynamical equations and use instead conservation of energy (i.e., constant H).
 
  • #6
Im just confused on how to use two initial conditions . Ray Vickson , what do you mean by the conservation of energy method?
 
  • #7
1670frank said:
Im just confused on how to use two initial conditions . Ray Vickson , what do you mean by the conservation of energy method?

Because of the form of the Hamiltonian, it is constant over time; that is, ##{\cal{H}}(t) \equiv H(p(t),x(t))## is constant. That means that for any t we have
[tex] p^2(t) - x^4(t) = p^2(0) - x^4(0) = 0.[/tex] Since the mass is 1 (from the form of H) we have
[tex] p(t) = \frac{d x(t)}{dt},[/tex]
so we get immediately a first-order DE for ##x(t)##.
 

FAQ: When Will the Particle Reach Infinity with Given Initial Values?

What is Hamiltonian flow?

Hamiltonian flow is a concept in physics and mathematics that describes the motion of a system over time. It is based on the Hamiltonian formalism, which uses a mathematical function known as the Hamiltonian to describe the energy of a system. The Hamiltonian flow is the path that the system takes as it evolves over time.

How is Hamiltonian flow related to Hamiltonian mechanics?

Hamiltonian flow is a fundamental concept in Hamiltonian mechanics, which is a branch of classical mechanics that uses the Hamiltonian formalism to describe the motion of a system. The Hamiltonian flow is the actual path that the system takes as it evolves according to the equations of motion derived from the Hamiltonian.

What is the significance of Hamiltonian flow in physics?

Hamiltonian flow is significant in physics because it provides a mathematical framework for understanding the dynamics of a system. It allows scientists to predict the future behavior of a system based on its initial conditions and the laws of physics. This is particularly useful in fields such as celestial mechanics, where the Hamiltonian flow can be used to accurately model the motion of planets and other celestial bodies.

How is Hamiltonian flow calculated?

The Hamiltonian flow is calculated using the equations of motion derived from the Hamiltonian. These equations take into account the system's initial conditions, such as position and velocity, as well as any external forces or constraints on the system. Numerical methods, such as Euler's method or the Runge-Kutta method, can be used to calculate the Hamiltonian flow for more complex systems.

What are some applications of Hamiltonian flow?

Hamiltonian flow has a wide range of applications in physics and mathematics. In addition to its use in celestial mechanics, it is also used in fields such as quantum mechanics, statistical mechanics, and fluid dynamics. It has also found applications in engineering, such as in the design of control systems for spacecraft and robots. Additionally, the concept of Hamiltonian flow has been extended to other areas of mathematics, such as symplectic geometry and the study of dynamical systems.

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