|
NE =
Signal excess, expressed in decibels (dB) as the ratio of signal to noise at the
system input above that required for reliable performance, and is a measure of
detection reliability.
|
|
LS =
Source level, a sound pressure expressed in dB referred to 1 dyne/ cm2
at a distance of 1 yard from the transducer
|
|
NW =
Total propagation loss (dB)
|
|
LN
= System noise level (dB)
|
|
NRD =
Required signal-to-noise ratio for display used (recorder, digitizer) (dB)
|
|
ND =
Two-way transmission loss in dome or other interface between the transducer and
the water (dB).
|
|
Source Level (LS)
|
|
|
|
The source level is the
sound pressure level (on axis) expressed in dB relative to 1 µbar at a distance of 1 yard
from the transducer. The source level is determined by:
|
|
n
The amount of electrical transmitting power applied to the transducer
|
|
n
The ability of the transducer to convert electrical energy to acoustical energy
in the water (i.e., transducer efficiency)
|
|
n
The ability of the transducer to concentrate the energy into a beam (i.e.,
transducer gain).
|
|
The above factors can be combined
in a logarithmic equation to give the source level
|
|
Equation -2
LS
= 71.6 + 10 log PE + N DIT
-E
|
|
where
|
|
PE
= Electrical transmitting power in watts (average pulse power).
|
|
|
|
E = Transducer
efficiency expressed in dB
|
|
NDIT
= Transducer transmitting directivity index.
|
|
71.6 = Parameter
conversion constant.
|
|
In addition, the
directivity index for a circular piston transducer can be calculated with a good
approximation by
|
|
Equation -3
|
|
where
|
|
A = Effective
radiating surface area of transducer in square inches
|
|

|
|

|
|
Propagation
Loss (NW )Propagation
Loss (NW )
|
|
There are two
basic propagation loss models, which can be used in the sonar equation to
calculate the depth capability of a bathymetric system. The difference between
the two models is based on the assumptions concerning the physics of the
reflection from the bottom. The first model considers the bottom echo to be
primarily a coherent signal reflection with a bottom loss factor to account for
absorption and scattering losses. This model is sometimes referred to as the
"lossy mirror" or "specula" model.
|
|
The second model
assumes no specularly reflected component, and the bottom reflected signal is an
incoherent addition of a large number of independent signal components. Each
unit element of the illuminated area contributes a small amount of reflected
signal power dependent on a back-scattering coefficient. In this case, the
reflected signal is a function of the illuminated area. This model is referred
to as the target strength or scattering model.
|
|
Specular Model
|
|
The propagation
loss is given by
|
|
Equation -4
|
|
where
|
|
NW
= Total propagation loss in decibels
|
|
R = Depth, yards
|
|
NBL
= Bottom loss caused by absorption and scattering.
|
|
Typical values of
bottom loss, NBL , at an operating frequency
of 12 kHz range from 10 to 30 dB, with value of 20 dB used for an average
value. For slope angles less than one half the acoustic beamwidth, there will be
a strong specular return and this first model applies.
|
|
Scattering Model
|
|
The propagation
loss for this model is
|
|
Equation -5
|
|
where
|
|
SB
= Bottom back scattering strength per unit area, a function of bottom slope.
|
|
A = Effective
illuminated area in square yards.
|
|
Measured values of back
scattering coefficient SB
are listed in Table 1. |