A cylindrical or a spherical pressure vessel, having inner diameter $d$ & thickness of wall $t$, is called thin if $\large \frac{t}{d}<\frac{1}{20}$.
$\bullet$ Thin cylindrical pressure vessel
hoop or circumferential stress $ \sigma_h=\large\frac{pd}{2t}$ & longitudinal stress $ \sigma_l=\large\frac{pd}{4t}$
$\bullet$ Thin spherical pressure vessel
hoop or circumferential stress $ \sigma_h=\large\frac{pd}{4t}$ & longitudinal stress $ \sigma_l=\large\frac{pd}{4t}$
In both the cases we consider only two stresses i.e. the system of plane stresses neglecting the radial stress $(\sigma_r)$.
The question is why do we neglect the radial stress for thin pressure vessels? Can it be explained by Lame's equation used for thick pressure vessels:
$$\sigma_h, \sigma_r=\frac{B}{x^2}\pm A\ \text{?}$$