We investigate the magnetic properties of the Cu-O planes in stoichiometric Sr\(_{n-1}\)Cu\(_{n+1}\)O\(_{2n}\) (n=3,5,7,...) which consist of CuO double chains periodically intergrown within the CuO\(_2\) planes. The double chains break up the two-dimensional antiferromagnetic planes into Heisenberg spin ladders with \(n_r=\frac{1}{2}(n-1)\) rungs and \(n_l=\frac{1}{2}(n+1)\) legs and described by the usual antiferromagnetic coupling J inside each ladder and a weak and frustrated interladder coupling J\(^\prime\). The resulting lattice is a new two-dimensional trellis lattice. We first examine the spin excitation spectra of isolated quasi one dimensional Heisenberg ladders which exhibit a gapless spectra when \(n_r\) is even and \(n_l\) is odd ( corresponding to n=5,9,...) and a gapped spectra when \(n_r\) is odd and \(n_l\) is even (corresponding to n=3,7,...). We use the bond operator representation of quantum \(S=\frac{1}{2}\) spins in a mean field treatment with self-energy corrections and obtain a spin gap of \(\approx \frac{1}{2} J\) for the simplest single rung ladder (n=3), in agreement with numerical estimates.