In order to investigate the effects of connectivity and proximity in the specific heat, a special class of exactly solvable planar layered Ising models has been studied in the thermodynamic limit. The Ising models consist of repeated uniform horizontal strips of width m connected by sequences of vertical strings of length n mutually separated by distance N , with N = 1, 2 and 3. We find that the critical temperature T c (N, m, n), arising from the collective effects, decreases as n and N increase, and increases as m increases, as it should be. The amplitude A(N, m, n) of the logarithmic divergence at the bulk critical temperature T c (N, m, n) becomes smaller as n and m increase. A rounded peak, with size of order ln m and signifying the one-dimensional behavior of strips of finite width m, appears when n is large enough. The appearance of these rounded peaks does not depend on m as much, but depends rather more on N and n, which is rather perplexing. Moreover, for fixed m and n, the specific heats are not much different for different N . This is a most surprising result. For N = 1, the spin-spin correlation in the center row of each strip can be written as a Toeplitz determinant with a generating function which is much more complicated than in Onsager's Ising model. The spontaneous magnetization in that row can be calculated numerically and the spin-spin correlation is shown to have two-dimensional Ising behavior.