A theoretical study is presented for a number N of Josephson junctions conn
ected as a one-dimensional (1D) parallel array in such a manner that there
an N-1 individual superconducting loops with arbitrary shape formed. In the
resistive array mode, for bias currents I>I-c, all Josephson junctions in
the array oscillate at the same magnetic held dependent frequency nu (B) wh
ich is, in general, not a Phi (0)-periodic function of the strength of magn
etic field B. Within the range of validity of the resistively and capacitiv
ely shunted junction (RCSJ) model the periodicity of nu (B) is controlled b
y the array geometry alone and does not depend on the distribution of the a
rray junction parameters. In the overdamped junction regime, nu (B) is for
certain types of unconventional grating structures a unique function around
a sharp global minimum at B=0. This filter property does not apply for reg
ular gratings and superconducting quantum interference devices (SQUID's). C
omputer simulations of the full nonlinear array dynamics reveal that the qu
alitative macroscopic quantum interference properties of unconventional arr
ays are governed, irrespective of the strength of inductive couplings, by a
complex structure factor S-N(B) which can be determined analytically. Also
, the performance of magnetometers based on ID arrays with unconventional g
rating structure can be significantly better than the performance of conven
tional SQUID's. In particular, ID arrays with unconventional grating struct
ure should provide a technically lather unsophisticated precision measureme
nt of absolute strength and orientation of external magnetic fields.