A length of coaxial cable radiates negligible amount of RF.
Same length, if cut into pieces of length (λ/2 * VF), and these pieces joined again cross-connected (i.e. core of a piece to shield of adjacent piece & vice versa), then this length of coax becomes a very good radiator of RF. Why & how?
EDIT on Feb 05, 2017:
Added sketch below to improve the question.