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Description  |
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BACKGROUND OF THE INVENTION
1. Field of the Invention
The invention relates to light responsive devices for developing an
electrical output signal indicative of movement or vibration and, more
particularly, but not by way of limitation, it relates to a motion sensing
device that is responsive to either absorption or fluorescence of light
radiation of predetermined wave lengths.
2. Description of the Prior Art
The prior art includes numerous types of motion sensing device which
function in response to variation in light transmission. A relatively
early form of seismic motion detector which was extremely sensitive to
earth vibrations utilizes a laser light source for effecting light
vibrations in response to extremely minimal vibrations as are detected and
amplified for further processing. The U.S. Pat. No. 4,155,065 is
considered to be of pertinence relative to the present invention as it is
the closest related art known to Applicant albeit that it is not really
anticipative of even the basic features of Applicant's invention. This
patent teaches the use of a liquid having ceramic particles dispersed
therein and utilizes the backscattering of laser energy to provide
detector indication of acoustic signals. In this case, the suspended
ceramic particles are oscillated by the impending acoustic waves at a
particular frequency whereupon the backscattered light is detected and
transformed into electrical signal output.
SUMMARY OF THE INVENTION
The present invention relates to an improved form of highly sensitive
motion sensing device which utilizes a light source and a selected dye
solution in order to provide detectable variations for producing an output
signal. More particularly, the device includes a sealed bag of fluid for
contacting and transmitting motion from a moving surface, which motion is
transposed through a light source and confined volume of the dye solution
to effect a variable light change. Such light change is then detected from
within a reaction mass member movably supported on said dye solution
enclosure which, in turn, produces an electrical signal indicative of the
motion for output and distribution.
Therefore, it is an object of the present invention to provide a high
sensitivity motion sensor.
It is also an object of the present invention to provide a seismic energy
detector which is easily coupled to an earth surface or downhole location
for vibration detection.
It is still further an object of the present invention to provide a
detector device that can be positioned in any selected angular disposition
to effect motion sensing.
Finally, it is an object of the present invention to provide a motion
detector device that relies upon changes in light absorption and/or
fluorescence to provide output data indication.
Other objects and advantages of the invention will be evident from the
following detailed description when read in conjunction with the
accompanying drawings which illustrate the invention.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a view in vertical section of a light effect sensor constructed
in accordance with the present invention;
FIG. 2 is a perspective view of the light effect sensor of FIG. 1 with
parts shown in cutaway;
FIG. 3 is another perspective view of the light effect sensor of FIG. 1
with still further sectional showing;
FIG. 4 is a perspective view of a light source member as constructed in
accordance with the present invention;
FIG. 5 is a graph of light intensity versus wavelength (in units of
nanometers) illustrating the absorption and fluorescence relationships for
one form of dye solution; and
FIG. 6 is a vertical section of an alternative form of light effect device
utilizing fiber optic interconnections.
DETAILED DESCRIPTION OF THE INVENTION
Referring to FIGS. 1-4, an acoustic energy sensor 10 is capable of
measuring either fluorescence or absorption quality in order to determine
the amplitude and frequency of acoustic signals. The sensor 10 can also
serve to measure pressure signal variations. The sensor 10 includes a
light source 12 as secured within such as a plexiglass block 14, in this
case a cylindrical block having end surfaces 16 and 18 and side surface
20.The plexiglass block 14 is highly polished on end surface 16 and side
surface 20 while end surface 18 is roughened to allow scattering light
transmission out of block 14. Any material having the requisite index of
refraction relative to the adjacent surface that will allow total internal
reflection may be used for block 14, e.g., Lexan.TM., lucite, etc.
A radial bore 22 is formed in block 14 to receive the light source 12 as
secured therein. Light source 12 may be such as a blue or green LED
energized via lead connection 24 as secured within bore 22 by means of a
suitable cement having the same or similar index of refraction as the
material of block 14. One suitable form of LED is a blue light emitting
diode which is available from Siemens Components, Inc., Opto Electronics
Division, Cupertino, Calif. This diode emits light over a wavelength range
from about 440 to 560 nanometers (nm) centered at about 500 nm. As cement
26 provides matching refractive index into block 14, all light will be
internally reflected within surfaces 20 and 16 since block 14 is selected
to be of more optically dense material (greater refractive index) than the
liquid 28 which is maintained adjacent the bottom surface 16, as will be
further described.
The liquid 28 is contained within a cowl-like member 30 secured about the
periphery of block 14. The cowl member 30 may be flexible, although it is
not absolutely necessary, and a flexible sealing membrane 32 is secured
over the outer, enlarged end of cowl member 30 to retain the liquid 28
therein. Liquid 28 and membrane 32 function to transmit any vibratory
movement of membrane 32 to the block 14, and any suitable acoustic
coupling liquid may be utilized as liquid 28, e.g., a glycerin-bas liquid
capable of exhibiting rapid dispositions.
The block 14 is secured adjacent a flexible dye reservoir 36 which includes
a light responsive dye liquid 38 contained therein. The reservoir 36 is
formed of flexible, transparent material to include an outer donut or ring
portion 40 and an inner central portion 42 (See FIG. 2) which consists of
circular transparent panels 44 and 46. The panels 44 and 46 are suitably
bonded to the flexible ring portion 40 in fluid-tight relationship.
Reservoir 36 allows for relative movement as between the upper and lower
reservoir panels 44 and 46, respectively.
The roughened, light transmissive surface 18 of block 14 emits light
through the transparent center panel 46 and into the dye liquid 38
whereupon both light absorption and fluorescence occurs, as will be
further discussed below. A thin coating of light filter material 48 may be
applied over light transmissive surface 18 to further define the bandwidth
or wavelength range of transmitted light into the dye liquid 38. Any light
indication from dye liquid 38 is then also transmitted into a block 50,
also a cylindrical, internally reflective member as formed from such a
plexiglas, lucite, Lexan.TM., etc., and which is highly polished to
contain internal light reflections on upper surface 52 and side surface
54. The bottom surface 56 is a roughened surface to allow light scatter
transmission from the reservoir top panel 44 into the block 50. A
restrictive light filter 58 may be employed to limit wavelength of light
passing between dye liquid 38 and the interior block 50.
The block 50 rests upon top panel 44 and an annular collar 60 formed from
such a metal is secured over the top surface 52 of block 50 to serve as a
reaction mass for effecting relative movement between the blocks 14 and 50
and, therefore, reservoir panels 44 and 46 thereby to modulate the volume
of dye liquid 38. Modulated light within block 50 can then only be
transmitted through a roughened surface area 62 to a photo-responsive
detector 64 disposed within a concentric bore 66 of collar 60. An
electrical output on lead 68 is input to further electronics 70, e.g., a
pre-amplifier or the like.
There are a number of dye substances that could be used as dye fluid 38 but
one that has been found particularly suitable is a dye known as
acriflavine. The acriflavine dye may be used in solution with a suitable
solvent such as ethanol or water in concentration on the order of
1.times.10.sup.-4 moles per liter. FIG. 5 illustrates the absorption curve
80 and the fluorescence curve 82 for acriflavine in terms of intensity
versus wavelength. The absorption curve 80 indicates a peak 84 at about
465 nanometers while the fluorescence curve 82 shows a peak 86 at about
500 nanometers. A suitable filter coating of 460-470 nm is illustrated by
shading 88 which intersects the absorption peak 84 and this filter coating
is particularly suitable for application as input filter 48 adjacent block
14. A second filter coating of 500-550 nm is shown by shading 90 may be
applied as output light filter 58 since it provides coverage of a good
portion of the higher spectral intensity values for the fluorescence curve
82 to allow passage into the block 50 and detector 64.
In operation in the absorption mode, and referring to FIG. 1, the light
source 12 is a light emitting diode emitting light in the 440-560 nm band
and this covers both the absorption and the fluorescence wavebands for the
acriflavine dye. Light emitted from source 12 is contained in block 14 and
passes through an absorption bandwidth filter layer 48 and the reservoir
panel 46 for travel through the dye liquid 38. Light not absorbed in dye
liquid 38 then passes through panel 44 and filter layer 58 to the detector
block 50 whereupon light output is seen through roughened surface 62 at
photo-responsive detector 64 to provide an output indication via lead 68.
In this case, filter layer 58 has the same spectral characteristics as
filter layer 48 so that it passes the same wave lengths of light.
The flexible diaphragm or envelope 32 is placed in contact with a ground
surface or other object of which vibrations are to be detected. Any such
vibration or movement at diaphragm 32 is transmitted through liquid 28 and
translated to block 14 through liquid dye 38, block 50, and reaction mass
60, thereby to vary the distance across liquid reservoir 36, i.e., between
panels 44 and 46. Thus, as the distance between panels 44 and 46 enlarges
or is made wider, more of the blue light is absorbed within dye liquid 38
to cause a corresponding decrease in light passing through filter layer 58
to the photo-responsive detector 64. That is, with an increase in width of
the dye liquid 38 there is an inverse or decreased detection of blue light
within the absorption band.
Thus, the output of the photo-responsive detector 64 will be a constant DC
value when no acoustic signal or motion is present at the diaphragm 32,
and when acoustic signal or movement is detected, the width of the active
dye region between panels 44 and 46 will increase and decrease in
response. Amplitude may be calibrated with known acoustic input signals to
the diaphragm 32, and the frequency can be determined by comparing
crossovers about the D-C value, or about zero if the electrical output is
A-C coupled. The amount of light absorption can be measured using the
relationship
I=I.sub.0 e.sup.-.sigma.A.spsp.N.sup.l (I)
where,
I=intensity of the transmitted light
I.sub.o =intensity of the incident light
.sigma.A=absorption cross section of the organic dye molecule in
centimeters squared (cm.sup.2)
N=number of molecules per centimeter cubed (cm.sup.3)
l=width of the active dye region in nanometers (nm)
Operating in the fluorescent mode, light from the source 12 within block 14
is emitted through a band limiting filter coating 48 in the range of
460-470 nm. Presence of this light within the acriflavine dye liquid 38
between movable panels 44 and 46 will cause fluorescence in the 500-550 nm
band and this light is transmitted through filter coating 58 which has a
wide pass band admitting the 500-550 nm wave lengths. This light is then
contained within light block 50 and presented through surface 62 to the
photo-responsive detector 64.
The mechanism for sensing motion is the change in fluorescence intensity
within dye liquid 38 due to a change in the width of the region of dye
fluorescence. That is, movement of liquid 28 causing narrowing between
panels 44 and 46 will cause a proportionate decrease in fluorescence and a
proportionate decrease in detected photoelectric signal. The fluorescence
mode works similar to the absorption mode except that the output detector
signal is directly proportional to the instantaneous width of the active
dye region between envelope panels 44 and 46. Fluorescence will occur in
accordance with PS
I.sub.F =I.sub.o e.sup..sigma.F.spsp.N.sup.l (2)
where,
I.sub.F =fluorescence intensity, and
.sigma.F=fluorescence cross section of the organic dye molecule in
centimeters squared.
Referring to FIG. 6, the device can be made electrically passive by using
fiber cable to channel light to and from the sensor device 10a. The light
block 14a is formed with a bore 92 which has a fiber optic cable 94
tightly secured therein. Light input, such as the selected LED diode
emitting blue light is provided at source 96 for injecting blue light of
the requisite band width through fiber optic cable 94 for internally
reflected containment within block 14a. The requisite filter coatings are
applied at surfaces 44 and 46 to allow either absorption or fluorescence
sensing from the liquid dye 38 between movable panels 44 and 46. Light
passed into light block 50a may then be transmitted along a fiber optic
cable 98 whereupon it is detected by a remote photo-responsive detector 64
and electrical signal is applied to electronics 70.
The remote location of the light source 96 and detector 64 may be desirable
for carrying out vibration sensing in particular seismic applications such
as at subsurface, downhole or other locations having difficult
accessibility. The foregoing discloses a novel motion detection device for
use in vibratory sensing or pressure monitoring applications. The
particular form of sensor device is quite versatile as it is capable of
adjustment and variation as regards the response parameters of the
acoustic coupling medium as well as the operating wavelength and selection
of pass band while operating in either the absorptive or the fluorescent
mode. The device is capable of being assembled in minute form while
exhibiting extreme rugged construction for use in any of a number of
varying types of situations.
Changes may be made in combination and arrangement of elements as
heretofore set forth in the specification and shown in the drawings; it
being understood that changes may be made in the embodiments disclosed
without departing from the spirit and scope of the invention as defined in
the following claims.
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Description  |
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