  We re-examine through an example the connection between the curvature of the
boundary of a set, and the decay at infinity of the Fourier transform of its
characteristic function. Let $B_p\subset\mathbb{R}^2$ denote the unit ball of
$\mathbb{R}^2$ in the $l^p$-norm. It is a consequence of a classical result of
Hlawka that for each $p\in(1,2]$, there exists $C(p)>0$ such that $$
|\widehat{\chi}_{B_p}(\omega)|\le
\frac{C(p)}{|\omega|^{3/2}}\quad(\omega\in\mathbb{R}^2, |\omega|\text{ large}).
$$ The above estimate does not hold for $p=1$. Thus, one expects that
$C(p)\rightarrow\infty$ as $p\rightarrow1+$; we determine the sharp asymptotic
behaviour of $C(p)$ as $p\rightarrow1+$.
