Imaging optical beam attenuation coefficient meter

Abstract

The present invention provides a meter and method of use for measuring an optical attenuation coefficient in a liquid medium. In operation, a collimated beam, produced by a laser of the attenuation meter apparatus, propagates thru the liquid medium with filtered back-scattered light arriving at a camera of the meter. A light image is formed at a focal plane of the camera. The light image is recorded and analyzed by a microcomputer to provide optical beam attenuations coefficients.

Claims

1. An attenuation meter for measuring optical attenuation in a liquid medium, said meter comprising: an optical window with a first and second section with said optical window being an outer section of said meter with said window separating an interior of said meter from the liquid medium; a continuous wave laser positioned as a first component within the interior with said continuous wave laser capable of projecting a collimated laser beam thru the first section of said optical window to the liquid medium with the result of backscattered light; an optical filter positioned interior to said optical window in said attenuation meter in which said filter is capable of only passing light at a wavelength of the laser beam from light which passes thru the second section of said optical window; a measuring device with a focal plane, with said measuring device positioned as a second component within the interior and with said measuring device capable of producing a light image passing thru said optical window and said optical filter onto said focal plane with the light image being an image of the backscattered light passed thru said optical filter; at least one sensor operationally connected to said focal plane wherein said sensor is capable of producing transmittable data based on the light image; and a microcomputer operationally connected to said sensor for receiving and analyzing the data for a beam attenuation coefficient.

2. The attenuation meter in accordance with claim 1, wherein said measuring device is a camera.

3. The attenuation meter in accordance with claim 2, wherein a focal length of said camera is based on an image size of the laser beam at a distance 1/(2c) where “c” is a beam attenuation coefficient.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) Other objects, features and advantages of the present invention will become apparent upon reference to the following description of the preferred embodiments and to the drawings, wherein corresponding reference characters indicate corresponding parts throughout the several views of the drawings and wherein:

(2) FIG. 1 depicts an operation of an attenuation meter of the present invention in a water environment;

(3) FIG. 2 presents a number of electrons within an image per pixel as a function of water range for an attenuation coefficient of c=1/(20 m), c=1/(10 m) and c=1/(5 m) with the number of pixels produced during the operation of the attenuation meter;

(4) FIG. 3 presents a number of electrons within an image per pixel as a function of a focal plane position for an attenuation coefficient of c=1/(20 m), c=1/(10 m) and c=1/(5 m);

(5) FIG. 4 presents a water range corresponding to a focal plane location;

(6) FIG. 5 presents a range resolution defined by a range extent covered by a single pixel along a focal plane as a function of a water range;

(7) FIG. 6 presents a total of electrons within a range cell given; and

(8) FIG. 7 presents a range cell to shot noise given by Equation (5).

DETAILED DESCRIPTION OF THE INVENTION

(9) An example of a measurement of a beam attenuation coefficient “c” is depicted in FIG. 1. In the figure, a modeled blue 473 nanometer beam is close to the wavelength of absorption in clear water. Also, a back scattering co-efficient used is approximate to that of natural waters. An assumed maximum range is approximately twelve meters. An attenuation meter 10 and a clear environment such as water 200 to be measured are shown.

(10) The attenuation meter 10 may be used with other liquid mediums. If used with other liquid mediums, the sensed backscattering could be based on density fluctuations in the liquid environment that produce an index of refraction.

(11) In operation, a continuous wave (CW) laser 12 produces a collimated laser beam 100 of a diameter D. As the laser beam 100 propagates thru the water 200, some of the propagated light becomes back-scattered light 102 arriving at the attenuation meter 10. This backscattered light 102 arrives at the meter 10 thru a back scattering of a thermodynamic index of refraction fluctuations and back scattering of particles within the water 200.

(12) A lens 16 of a camera 14 within the attenuation meter 10 uses the backscattered light 102 from the laser beam 100 to form a light image of the laser beam on a tilted focal plane of the camera. Sensors 18 on the focal plane detect the light image. The light image extracts a measurement of the optical beam attenuation coefficient “c” at the wavelength of the laser beam 100. The sensors 18 then transmit data based pixels of the light image to a microcomputer 20. The microcomputer 20 controls the function of the attenuation meter 10 as well as providing analysis of the recorded light image.

(13) An optical window 22 separates the attenuation meter 10 from the water 200 and an optical filter 24 rejects background light by only passing light at the wavelength of the laser beam 100.

(14) Rectangular coordinates (x, y), shown in FIG. 1, are used for selection of parameters. The conditions and definitions entitled “Example” on FIG. 1 are modeled and the results are presented in FIGS. 2-7. To provide adequate measurement accuracy, a maximum water range is chosen to be one half of an expected maximum attenuation length l/c. The expected maximum attenuation length would be obtained from published data of environmental characteristics.

(15) Also, the beam diameter “D” should be large enough to maintain beam collimation over 1/(2c) but not larger than ½ (1/c) in order to minimize the contribution of forward scattering that falls within the collimated beam in the measurement (i.e. the maximum forward scattering).

(16) A focal length of the lens 16 is chosen so that the image size of a beam at the distance 1/(2c) exceeds the sensor pixel size for realistic pixel (4-20 microns) and focus plane sizes (0.5-2 microns). Using the definitions in FIG. 1, the number of detected electrons within the image per pixel is calculated by Equation (1) with the number of electrons being the signal strength that is recorded.

(17) $\begin{array}{cc}N\cong \frac{{\mathrm{QTPte}}^{\left(-2{\mathrm{cy}}_w\right)}\beta \left(180°\right){{\mathrm{AA}}_{\mathrm{pix}}\left(y_a-f\right)}^2}{E_{\mathrm{photon}}{n}^2{f}^2{D\left(x_0^2+f^2\right)}^{0.5}{\left(x_0^2+y_a^2\right)}^{0.5}}& \left(1\right)\end{array}$
where “P” is the laser power; “Q” is the sensor quantum efficiency; “T” is the system transmission co-efficient, “n” is the water index of refraction; “A” is the entrance pupil area; A.sub.pix is the area of a pixel; “E.sub.photon” is the energy of a photon; and “f” is the lens focal length.

(18) FIG. 2 depicts the number of electrons “N” as a function of water range for an attenuation coefficient of c=1/(20) meters, c=1/(10) meters, and c=1/(5) meters. The figure clearly shows that the shapes for varying values of beam attenuation are very different. Thus, fitting the shape of experimental results to those predicted by Equation (1) will produce a measurement of the beam attenuation coefficient, c.

(19) FIG. 3 presents the same results as a function of focal plane position. FIG. 4 presents the water range, y.sub.w, corresponding to focal plane location, S, and f is the focal length given by

(20) $\begin{array}{cc}S=\frac{{f\left(x_0^2+f^2\right)}^{0.5}}{\left(y_w-f\right)}& \left(2\right)\end{array}$

(21) FIG. 5 presents the range resolution “r” defined by the range extent covered by a single pixel along the focal plane as a function of water range given by:

(22) $\begin{array}{cc}r=\frac{n{\mathrm{pix}\left(y_w-f\right)}^2}{{f\left(x_0^2+f^2\right)}^{0.5}}& \left(3\right)\end{array}$
where “n” is the indexed refraction and “pix” is the pixel size.

(23) Summing over a transverse image extent (beam size perpendicular to the plane of FIG. 1), the total elections within a range cell is given by

(24) $\begin{array}{cc}{N}_{\mathrm{TOTAL}}=\frac{\mathrm{NDF}}{y_w\mathrm{pix}}& \left(4\right)\end{array}$

(25) The results of applying Equation (4) are presented in FIG. 6. FIG. 7 presents a “signal-to-shot noise” given by Equation (5).
Signal to shot noise=(N.sub.TOTAL).sup.0.5  (5)

(26) An advantage of the present invention is the ability to obtain measurements over long propagation paths and therefore provide accurate measurements of optical beam attenuation coefficients. Another advantage of the invention is that relatively low cost power continuous wave lasers are used rather than short duration pulsed lasers.

(27) The attenuation meter 10 can be deployed as a self-contained module and can be powered by batteries. Furthermore, the attenuation meter 10 can be deployed on vehicles such as unmanned underwater vehicles or deployed from a separate platform with an umbilical cable that supplies electrical power and access to stored data and results. The attenuation meter can contain more than one color light source to provide measurements at more than one wavelength.

(28) The foregoing description of the preferred embodiments of the invention has been presented for purposes of illustration and description only. It is not intended to be exhaustive nor to limit the invention to the precise form disclosed; and obviously many modifications and variations are possible in light of the above teaching. Such modifications and variations that may be apparent to a person skilled in the art are intended to be included within the scope of this invention as defined by the accompanying claims.