In physics, and more specifically in Hamiltonian mechanics, a generating function is, loosely, a function whose partial derivatives generate the differential equations that determine a system's dynamics. Common examples are the partition function of statistical mechanics, the Hamiltonian, and the function which acts as a bridge between two sets of canonical variables when performing a canonical transformation.

In canonical transformations

There are four basic generating functions, summarized by the following table: ^[1]

Generating function	Its derivatives
${\displaystyle F=F_{1}(q,Q,t)\,\!}$	${\displaystyle p=~~{\frac {\partial F_{1}}{\partial q}}\,\!}$ and ${\displaystyle P=-{\frac {\partial F_{1}}{\partial Q}}\,\!}$
${\displaystyle F=F_{2}(q,P,t)=F_{1}+QP\,\!}$	${\displaystyle p=~~{\frac {\partial F_{2}}{\partial q}}\,\!}$ and ${\displaystyle Q=~~{\frac {\partial F_{2}}{\partial P}}\,\!}$
${\displaystyle F=F_{3}(p,Q,t)=F_{1}-qp\,\!}$	${\displaystyle q=-{\frac {\partial F_{3}}{\partial p}}\,\!}$ and ${\displaystyle P=-{\frac {\partial F_{3}}{\partial Q}}\,\!}$
${\displaystyle F=F_{4}(p,P,t)=F_{1}-qp+QP\,\!}$	${\displaystyle q=-{\frac {\partial F_{4}}{\partial p}}\,\!}$ and ${\displaystyle Q=~~{\frac {\partial F_{4}}{\partial P}}\,\!}$

Example

Sometimes a given Hamiltonian can be turned into one that looks like the harmonic oscillator Hamiltonian, which is

${\displaystyle H=aP^{2}+bQ^{2}.}$

For example, with the Hamiltonian

${\displaystyle H={\frac {1}{2q^{2}}}+{\frac {p^{2}q^{4}}{2}},}$

where p is the generalized momentum and q is the generalized coordinate, a good canonical transformation to choose would be

${\displaystyle P=pq^{2}{\text{ and }}Q={\frac {-1}{q}}.\,}$

(1)

This turns the Hamiltonian into

${\displaystyle H={\frac {Q^{2}}{2}}+{\frac {P^{2}}{2}},}$

which is in the form of the harmonic oscillator Hamiltonian.

The generating function F for this transformation is of the third kind,

${\displaystyle F=F_{3}(p,Q).}$

To find F explicitly, use the equation for its derivative from the table above,

${\displaystyle P=-{\frac {\partial F_{3}}{\partial Q}},}$

and substitute the expression for P from equation ( 1), expressed in terms of p and Q:

${\displaystyle {\frac {p}{Q^{2}}}=-{\frac {\partial F_{3}}{\partial Q}}}$

Integrating this with respect to Q results in an equation for the generating function of the transformation given by equation ( 1):

${\displaystyle F_{3}(p,Q)={\frac {p}{Q}}}$

To confirm that this is the correct generating function, verify that it matches ( 1):

${\displaystyle q=-{\frac {\partial F_{3}}{\partial p}}={\frac {-1}{Q}}}$

See also

• Hamilton–Jacobi equation
• Poisson bracket

References

Further reading

• Goldstein, Herbert; Poole, C. P.; Safko, J. L. (2001). Classical Mechanics (3rd ed.). Addison-Wesley. ISBN  978-0-201-65702-9.