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| − | The '''Hamiltonian''' is a quantity of great importance in both classical and quantum mechanics. | + | The '''Hamiltonian''' is a quantity of great importance in both [[classical mechanics|classical]] and [[quantum mechanics]]. |
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| | == Classical mechanics == | | == Classical mechanics == |
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| | <math>H=\sum_i p_i \dot{q_i} - L </math> | | <math>H=\sum_i p_i \dot{q_i} - L </math> |
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| − | where <math>q_i</math> are the generalised co-ordinates and <math>p_i</math> are the [[momentum|momenta]] conjugate to these co-ordinates, and <math>L</math> is the [[Lagrangian]]. For many problems the Hamiltonian is the same as the energy. | + | where <math>q_i</math> are the generalised coordinates and <math>p_i</math> are the [[momentum|momenta]] conjugate to these coordinates, and <math>L</math> is the [[Lagrangian]]. For many problems the Hamiltonian is the same as the energy. |
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| | ===Example=== | | ===Example=== |
| − | For a mass <math>m</math> attached to a spring of spring constant <math>k</math> extended by a distance <math>x</math>, <math>L=m\dot{x}^2/2-kx^2/2</math> and so | + | For a [[mass]] <math>m</math> attached to a [[spring]] of [[spring constant]] <math>k</math> extended by a distance <math>x</math>, <math>L=m\dot{x}^2/2-kx^2/2</math> and so |
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| | <math> | | <math> |
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| | </math> | | </math> |
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| − | which is the familiar expression for the energy of a simple harmonic oscillator. | + | which is the familiar expression for the energy of a simple [[harmonic oscillator]]. |
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| | == Quantum mechanics == | | == Quantum mechanics == |
| − | The Hamiltonian for many quantum mechanical systems can be obtained by writing down a corresponding classical Hamiltonian and promoting all of the co-ordinates and momenta to operators. The quantum mechanical Hamiltonian is of central importance to the [[Schrodinger equation]]. | + | |
| | + | The Hamiltonian for many quantum mechanical systems can be obtained by writing down a corresponding classical Hamiltonian and promoting all of the coordinates and momenta to operators. The quantum mechanical Hamiltonian is of central importance to the [[Schrodinger equation]]. |
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| | [[Category:Physics]] | | [[Category:Physics]] |