ಉಷ್ಣವಲಯದ ಅಮೇರಿಕನ್ ಆರ್ಕಿಡ್‌ಗಳ ಕುಲ,

miltonia ಕನ್ನಡದಲ್ಲಿ ಉದಾಹರಣೆ:

ಟೆಕ್ಟೋನ ಹ್ಯಾಮಿಲ್ಟೋನಿಯಾನ (Tectona hamiltoniana).

miltonia's Usage Examples:

Example type IIIn the Hamiltonian formalism of the type II Painlevé equation\displaystyle y^{\prime\prime}2y^3+ty+b-1/2with\displaystyle qy,py^\prime+y^2+t/2two Bäcklund transformations are given by\displaystyle (q,p,b)\rightarrow (q+b/p,p,-b)and\displaystyle (q,p,b)\rightarrow (-q, -p+2q^2+t,1-b).

Alternative formulation Equivalent expressions are obtained by a slightly different partitioning of the Hamiltonian, which results in a different division of energy terms over zeroth- and first-order contributions, while for second- and higher-order energy corrections the two partitionings give identical results.

See also Energy driftMultisymplectic integratorVariational integratorVerlet integration References Numerical differential equationsHamiltonian mechanics Emilio Lunghi (16 March 1887, in Genoa "ndash; 27 September 1925) was an Italian athlete.

The JT HamiltonianEigenvalues of the Hamiltonian of a polyatomic system define PESs as functions of normal modes Q_i of the system (i.

+ \hat{H}_{6} ,in which the consecutive partial operators are:\hat{H}_{0} \sum_{i}\frac{\hat{p}_{i}^{2}}{2m_{i}} + V is the nonrelativistic Hamiltonian (m_{i} is the stationary mass of particle i).

An example is the spectral line splitting in the Zeeman effect, due to a magnetic interaction perturbation in the Hamiltonian of the atoms involved.

Using the action principle, a Lagrangian can be constructed from the trace of a polynomial function of these matrices, leading to Hamiltonian equations of motion.

\qquad\qquad (1)This happens frequently in Hamiltonian mechanics, with T being the kinetic energy and V the potential energy.

Misner) is a Hamiltonian formulation of general relativity that plays an important role in canonical quantum.

ProofThis proof of the Hellmann–Feynman theorem requires that the wavefunction be an eigenfunction of the Hamiltonian under consideration; however, one can also prove more generally that the theorem holds for non-eigenfunction wavefunctions which are stationary (partial derivative is zero) for all relevant variables (such as orbital rotations).

Furthermore, since the Hamiltonian is a [operator], the H matrix is also [matrix|hermitian] and the values of \varepsilon_i will be real.