The leading asymptotic terms of small-angle slit-smeared intensities, at la
rge momentum transfer h = (4 pi/lambda)sin (theta/2), are obtained from the
pinhole intensities by an integral transform whose kernel is the beam-heig
ht profile determined by the slits used in a Kratky camera. This profile, d
irectly measurable, generally shows a trapezoidal shape characterized by Q(
0), the end point of its horizontal plateau, and Q(1), the momentum-transfe
r value beyond which it vanishes. It results that any pinhole contribution,
monotonically decreasing as 1/h(alpha), after being smeared, decreases as
1/h((alpha-1)) in the region h < Q(0), while the power exponent monotonical
ly increases from (alpha - 1) to alpha in the outer h region. The actual ch
ange explicitly depends on the slit length. On the contrary, the oscillator
y damped contributions cos(h delta)/h(4) and sin(h delta)/h(4), after being
smeared, remain close, whatever the slit length, to those resulting from t
he smearing with an ideal slit.