We calculate the dependence of the transverse coupling losses in cable
s, the most important contribution to ac losses in cables without cent
ral insulating layer, Two effects cause differences with respect to th
e infinite samples: 1) changed area of the loops between the strands,
and 2) increased resistivity between them, At low frequencies, the tra
nsverse losses P for finite samples of length l are well-described by
the formula P/P-infinity = 1 - C(0)l(0)/l, where C-0 depends on the ra
tio b/c (b-cable width, c-thickness of normal layer between strands),
l(0) is the cabling length and P-infinity the losses for corresponding
infinite sample, We obtain a = 1/C-0 approximate to 3 for b/c approxi
mate to 10 and a approximate to 2 for b/c > 50. The same formula appli
es for higher frequencies, with frequency dependent correction factor
C(omega). This correction factor decreases and becomes even negative a
t higher frequencies, Thus, the losses in finite samples are higher th
an in the corresponding infinite cables, This effect could be therefor
e called the inverse size effect, appearing above omega tau > 0.9 for
b/c = 10 and omega tau > 1.53 for b/c = 50. It may explain some experi
mental results where size effect was expected but not found in the los
s measurements.