Low frequency, log-periodic acoustic array
AssigneeThe United States of America as represented by the Secretary of the Navy
InventorFrank W. Cuomo
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Abstract
A method for determining optimum element spacing for a low frequency, log-periodic acoustic line array comprising a plurality of omnidirectional hydrophones arranged in a line wherein the spacing between hydrophones is based on a logarithmic relationship using multiple dipole pairs, each pair centered about the acoustic axis of the array, such that the distance between each dipole pair bears a constant ratio to the wavelength of the acoustic frequency band to be investigated by that hydrophone pair. Each dipole pair relates to a particular frequency band and the assembled array covers at least a decade range of frequencies through juxtaposition of contiguous frequency bands. The overall arrangement assures retention of selected beam pattern directionality over the entire decade range of frequencies.
Claims1
A method of determining the sequential dipole spacing of a plurality of hydrophone dipole pairs about an array acoustic axis so as to form a low frequency, log-periodic acoustic line array wherein the acoustic beam pattern formed by each independent dipole pair has a quasi-constant directionality over a frequency band and the assembled array covers at least a decade range of frequencies through juxtaposition of contiguous frequency bands, said method comprising the steps of:
- selecting an operational frequency range;
- determining the spacing (2d.sub.n) of the innermost dipole pair using the following relationship
- 2 d.sub.n =(c/f) (A)
- wherein d.sub.n is the distance of each dipole element from the array acoustic axis, c is the speed of sound in seawater at the operational frequency, temperature and pressure the array will experience and f is the maximum desired operational frequency;
- selecting a minimum null depth commensurate with desired directionality descrimination;
- selecting a (d/.lambda.).sub.max for the ideal null from a graph wherein d equals 2d.sub.n and represents the distance between dipole pairs and .lambda. is the wavelength of the associated acoustic frequency;
- selecting a (d/.lambda.).sub.min from said graph for said minimum null depth;
- solving the following relationship for .tau. ##EQU8## wherein .tau. is an arbitrary constant associated with the log-period;
- solving the following relationship for d.sub.n-1 ##EQU9## using .tau. from (B) supra;
- repeating (C) supra iteratively substituting the previous d.sub.n-1 result for d.sub.n in (C) and solving for new d.sub.n-1's until 2d.sub.n, 2d.sub.n-1, etc. spacing for a frequency decade has been described;
- and
- arranging said hydrophones in accordance with said 2d.sub.n, 2d.sub.n-1, etc. spacing.
Dependencies are inferred from the claim text.