We study the a.c. transport through a two-dimensional quantum point co
ntact (QPC) using a Boltzmann-like kinetic equation derived for the pa
rtial Wigner distribution function. An integral equation for a potenti
al inside a QPC is solved numerically. It is shown that the electric f
ield inside a QPC is an inhomogeneous function of the spatial coordina
te, with a characteristic scale equal to the distance between the elec
tron's turning points. A dependence of the admittance on the frequency
of the a.c. field is found in the frequency range, omega approximate
to 0-50 GHz. The contribution to the imaginary part of the admittance
due to the open and closed channels is numerically calculated. It is s
hown that the crossover of quantum capacitance and quantum inductance
from localized behaviour to distributed behaviour takes place at omega
similar to 10 GHz. A transition from 2D plasmons to quasi-1D plasmons
is analysed as a function of two dimensionless parameters: k(x)d(0) (
where k(x) is the longitudinal wavevector and do is the width of the Q
PC) and the number of open electron channels, N.