  It is explicitly shown that either the approximate solution of the integral
equation for the inverse of the pion form factor, or the result of the Pad\'e
approximant method of resumming the one loop Chiral Perturbation Theory (CPTH)
are equivalent to the standard vector meson dominance (VMD) models, using the
vector meson coupling to two pseudoscalars given by the KSRF relation.
Inconsistencies between the one loop CPTH and its unitarised version (or the
VMD model) are pointed out. The situation is better for the CPTH calculation of
the scalar form factor and the related S-wave $\pi \pi$ scattering. The
branching ratios of $\tau \to \pi^+ \pi^0 \nu$, $\tau \to K \pi \nu$, $\tau \to
K^+ \eta \nu$ and $\tau \to K^+ \bar{K^0} \nu$ using only two inputs as the
$\rho $ and $K^*$ masses, or the two corresponding rms radii, agree with the
experimental data. Using the same number of parameters, the corresponding one
loop CPTH calculation cannot explain the $\tau$ data.
