Immersion Refractometer

Abstract

A device for measuring the absolute value of the refractive index of a liquid by immersion uses the optical properties of a cylindrical waveguide with a solid core and normal angle of incidence of the light source. The device consists of a transparent tube forming the enclosure of the waveguide, impervious to the surrounding liquid and partially filled with a transparent solid or liquid material of appropriate index of refraction, a fiber optic means of inputting light via a LED or laser and fiber optic means of coupling emerging light to a photodetector. The emerging light intensity is a function of the index of refraction of the surrounding liquid.

Claims

1. A device for measuring the refractive index of a liquid comprising a transparent tube partially filled with a solid or liquid transparent material, a fiber optic means of inputting light via an LED or laser and a fiber optic means of coupling emerging light to a photodetector such that the input light and emerging light are at the same end of the tube.

2. The device in claim 1 wherein the tube is made of quartz or other high index transparent material such that its refractive index is much greater than the transparent fill material to minimize the effects of the tube enclosure.

3. The device of claim 1 wherein the tube that is of sufficient length to subtend the liquid such that the active region is fully immersed.

4. The device of claim 1 wherein the transparent tube filling material consists of air or gas with sufficiently low refractive index that renders the device insensitive to refractive index changes of the surrounding liquid such that liquid level sensing via Fresnel reflections along the axis of the tube can be affected.

5. The device of claim 1 wherein the refractive index of the tube filling material is equal to or exceeds the upper limit of the refractive index range of the surrounding liquid as described in FIG. 1 and is appropriate to a specific application such as battery state of charge sensing, sugar content of certain distillates, sugar content of urine, anti freeze concentrations and other specific applications where refractive index is significant in the monitoring or manufacturing of liquids.

6. The device of claim 1 wherein the fiber optic means of inputting and outputting light fibers are comprised of one or more fibers bundled together within a ferrule is such that light enters and exits at the same end of the device.

7. The device of claim 1 further comprising a reflecting mirror at the end of the tube positioned orthogonally to the optical axis of the tube such that the incident light traverses the core region twice effectively increasing the active length by a factor of 2.

8. The device of claim 6 wherein the input fiber bundle is parallel to the tube axis without regard to specific angle of impingement on the interface between the guide and the solid material.

9. The device of claim 1 further comprising an enclosure that is mechanically compatible with open port batteries.

10. The device of claim 1 further comprising a small temperature sensing element such as a thermocouple or thermistor inserted within the ferrule to enable the monitoring of liquid temperature thus allowing correction of the variation of the index of the surrounding liquid with temperature.

11. The device of claim 6 wherein the tube ferrule enclosing the fiber bundle is made with a light absorbing material to minimize the effects of Fresnel reflections between the ferrule and the tube wall beyond the active length of the probe.

12. The device of claim 1 wherein the light source operates in the IR with wavelengths >700 nm to minimize ambient light interference.

13. The device of claim 1 whereas the fiber optic means by which the light enters the tube material is through an optical window separating the material and the fiber bundle.

14. The device of claim 1 wherein an electronic self calibration may be affected by using the refractive index of air as a calibration standard.

15. The device of claim 1 further comprising a battery, microprocessor and display such that the output of the device may be converted and displayed in calibrated engineering units appropriate to the specific application as shown for example in FIGS. 6,7.

16. The device of claim 1 wherein a practical embodiment of the device may be used in battery powered vehicles as a fuel gauge.

17. The device of claim 1 wherein a practical embodiment of the device may be used in battery monitoring systems for function assurance.

18. The device of claim 1 wherein a practical embodiment of the device may be used in battery charging systems for precision charging control.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0020] FIG. 1 is a graphical description of the relative change in output signal of the device as a function of the core index and the surrounding liquid index to be measured. It is shown for two different core indices and represents the actual phenomenology on which this invention is based.

[0021] FIG. 2 is a depiction of the major components of the device.

[0022] FIG. 3 shows the physical construction of the ferrule assembly containing the fiber optic bundles that input light into the device and output light to the photodetector.

[0023] FIG. 4 shows the means by which a small thermocouple, thermistor or RTD may be inserted within the ferrule to measure the temperature of the surrounding liquid.

[0024] FIG. 5 shows an alternate configuration of the device as implemented in a cell of a typical lead acid battery.

[0025] FIG. 6 shows an alternate configuration of the device as implemented in a portable battery powered unit with digital display.

[0026] FIG. 7 is a graphical description of the means by which the device may be calibrated in terms of engineering units appropriate to the specific application.

DETAILED DESCRIPTION OF THE INVENTION

[0027] FIG. 1 is a graph of the response of the device as a function of the core index and surrounding liquid refractive index. This graph illustrates a general trend of performance and the requirement to tune the refractive index of the core for compatibility of the liquid indices to be measured. This figure represents the phenomenological results on which this invention is based

[0028] The preferred configuration of the invention for the measurement of the refractive index of a liquid by immersion is shown in FIG. 2. and consists of: [0029] a. Light source 1 such as a LED or laser. [0030] b. A fiber optic means 2 of conveying the light source to the tube surrounding the core [0031] c. A tube 3, impervious and resistant to the surrounding liquid,d whose optical properties do not impact the basic operating principle of the device [0032] d. An active length and diameter 4 of the tube filled with a transparent solid 5 of appropriate index [0033] e. An end-mirror 6 to reflect the light back toward the input increasing the effective length [0034] f. A fiber optic means 7 of conveying the reflected light to a conventional photodetector [0035] g. A photodetector 8 to convert the reflected light to a electrical signal

[0036] The performance of this device in terms of the signal loss during propagation is a function of tube material, core index, liquid index, tube diameter, tube length, wavelength of the incident light and the numerical aperture of the input source. As the surrounding liquid changes its refractive index the amount of power transmitted through the device changes accordingly thus illustrating the basic principle of operation.

[0037] The choice of the tube material is dependent on 3 properties: impervious to the surrounding liquid, the transparency of good quality glass, and of refractive index such that the tube does not impact the basic performance expressed by Eq. 1. This latter property is achieved by choosing a refractive index that is much greater than the core index such as glass, pyrex or preferably quartz with index 1.54 at 590 nm. With a tube material index much greater than the core index the conditions for confined rays expressed by Eq. 1 are violated and the tube becomes totally transparent in a waveguide sense relying only on the liquid index to determine the propagation characteristics.

[0038] The choice of tube length depends on the tolerable signal loss and the tube diameter. Longer tubes yield more loss because the incident light undergoes more reflections as the light propagates down the tube. The preferred embodiment yields an effective tube length of approximately 2. Length acts in consonance with tube diameter to yield the actual loss as a function of the surrounding liquid index.

[0039] The choice of tube diameter is a function of the numerical aperture of the tube input fiber combination. In the configuration above the core region will only propagate light that enters the tube within a certain cone known as the acceptance angle. Eq. 1 can be re-expressed as

n sin .sub.max={square root over (n.sub.co.sup.2n.sub.cl.sup.2)}(2) [0040] where n is the refractive index of the entry medium, n.sub.co is the refractive index of the core, and n.sub.cl is the refractive index of the cladding as before.

[0041] Light entering the core at angles greater than sin .sub.max will not undergo total reflection and thus those rays will not be transmitted through the core of the device. In this form, the quantity n sin .sub.max is defined as the numerical aperture (NA) of the system. The number of reflections that a ray undergoes as it traverses the tube is a function of the tube diameter. For a given NA of the entry fibers, larger diameter tubes yield fewer reflections and less loss during propagation.

[0042] The number of modes supported by a cylindrical waveguide or optical fiber is proportional to the diameter D of the fiber and given as:

[00001]$\begin{array}{cc}N=\frac{.Math..Math.D}{}.Math.\sqrt{n_{\mathrm{co}}^2-n_{\mathrm{cl}}^2}& \left(3\right)\end{array}$

[0043] where is the wavelength of light.

The more modes a waveguide is capable of supporting the more power is transported from a multi-mode source.

[0044] For a given index of core material, the tube length and diameter work in consonance to yield a certain loss per unit length. There are no reliable analytical predictions of this relationship however in the preferred embodiment of this device with a core material index of 1.38, a tube length of 25 mm and a core diameter of 2 mm yields excellent performance over a liquid index range of 1.36 to 1.38.

[0045] The optical assembly whereby the light may be conveyed in and out of the tube is shown in FIG. 3. The optical assembly consists of a multiplicity of optical fibers encased in a ferrule 9 consisting of independent bundles 10 for both the light input 11 ferrule by way of LED or laser and output light ferrule 14 to a photodetector. The composite ferrule 9 may be of a light absorbing material to minimize anomalous waves travelling between the ferrule body and the tube which may disturb the readings. The input light emerging from the central ferrule 12 is incident normal to the surface of the solid material that comprises the core of the fiber. The principal feature of this assembly is that the light is effectively double passed by means of an end mirror 13 through the active medium thus increasing the effective length and hence the sensitivity of the device.

[0046] An alternate configuration of the device shown in FIG. 4 can be used to measure the temperature of the surrounding liquid in addition to the refractive index by inserting a small thermocouple or thermistor, thermocouple or RTD 16 within the fiber bundle 15.

[0047] An alternate configuration of the device suitable for insertion into an open port of a conventional lead-acid storage battery cell 20 is shown in FIG. 5. The active region of the tube containing the solid material is immersed in the battery electrolyte 21. The flanged bayonet mounting 19 is designed to be mechanically compatible with the most conventional storage batteries. The cap assembly 17 contains an electronics board 18 containing the light source, photodetector and processing electronics.

[0048] An alternate configuration of the device implemented in a hand-held, battery powered portable device is shown in FIG. 6. This embodiment may be calibrated in terms of suitable engineering units such as specific gravity and displayed 22 using a LCD or LED device.

[0049] The device may be calibrated as shown in FIG. 7 in terms absolute value of the refractive index or other engineering units related to refractive index by using a series of standard calibration solutions and a curve fitting algorithm such as a polynomial fit to yield accurate values of the units as a function of the output voltage of the photodetector. This technique circumvents such problems as dispersion effects due to the use of differing light source wavelengths.