Hamiltonian as total energy for natural systems?

In summary, the proof of H=T+V for systems with time-independent transformation from Cartesian to Generalized coordinates relies on expressing the kinetic and potential energies in terms of the generalized coordinates and their derivatives. Since the transformation is time-independent, the energies can be expressed without any explicit dependence on time, leading to the conclusion that the total energy H is equal to the sum of kinetic and potential energies. This has been demonstrated through the use of mass matrix components and generalized coordinates.
  • #1
CrazyNeutrino
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Could someone please prove that the H=T+V for systems where the transformation from Cartesian to Generalized coordinates is time independent. I have read through the proofs in Taylor's classical mechanics and Goldstein's but do not understand them.
 
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  • #2
Thanks in advance.The proof of this statement relies on the fact that the kinetic energy and potential energy can be expressed in terms of the generalized coordinates and their derivatives. In general, the kinetic energy is given by:T = ½m i θi·2 + ½m ij θi θj·2 + ½m ijk θi θj θk·2 + ...where m i , m ij , m ijk , ... are the components of the mass matrix and θi , θj , θk , ... are the generalized coordinates. Similarly, the potential energy is given by:V = V(q1, q2, ..., qn)where q1, q2, ..., qn are the generalized coordinates. Now, since the transformation from Cartesian to Generalized coordinates is time independent, the kinetic energy and potential energy can be expressed as functions of the generalized coordinates only, without any explicit dependence on time. This means that the total energy H of the system is given by:H = T + V where T and V are the kinetic and potential energies expressed in terms of the generalized coordinates, as above. Thus, we have shown that the total energy of a system where the transformation from Cartesian to Generalized coordinates is time independent is given by H = T + V.
 

Related to Hamiltonian as total energy for natural systems?

1. What is the Hamiltonian as total energy for natural systems?

The Hamiltonian is a mathematical construct used in physics to describe the total energy of a physical system. It includes the system's potential and kinetic energies, as well as any other relevant energy terms.

2. How is the Hamiltonian used in natural systems?

In natural systems, the Hamiltonian is used to describe the dynamics of the system over time. It is used to make predictions about the behavior and evolution of the system, based on its total energy and other relevant factors.

3. What is the relationship between the Hamiltonian and the laws of conservation of energy and momentum?

The Hamiltonian is closely related to the laws of conservation of energy and momentum. In fact, the Hamiltonian is conserved in any system where these laws hold true. This means that the total energy of the system, as described by the Hamiltonian, remains constant over time.

4. How is the Hamiltonian calculated for a natural system?

The Hamiltonian is calculated using mathematical equations and principles, such as the Lagrangian formalism and the Hamiltonian equations of motion. These equations take into account the physical properties and interactions of the system's components to determine its total energy.

5. Can the Hamiltonian be used to describe all natural systems?

While the Hamiltonian is a powerful tool for describing many natural systems, it is not applicable to all systems. Certain complex systems, such as those involving quantum mechanics or relativity, may require different mathematical approaches to accurately describe their total energy and dynamics.

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