Low radiation densitometer

Claim 2

Apparatus for measuring fluid density comprising, in combination: a source of radiation operable to emit radiation generally along a first path; first and second radiation detectors each operable to produce an output signal indicative of the radiation received thereby; means mounting the source and the radiation detectors in the fluid whose density is to be measured with the first detector in the first path at a first distance from the source and the second detector in the first path at a second distance from the source; and ratio means connected to the radiation detectors to receive the output signals therefrom and to produce a ratio signal which varies with the density of the fluid.

Claim 3

Apparatus according to claim 1 further including computing means connected to the ratio means to receive the ratio signal and operable to produce a resultant signal indicative of the density of the fluid.

Claim 4

Apparatus according to claim 2 further including indicator means connected to the computing means to receive the resultant signal.

Claim 5

Apparatus according to claim 1 wherein the source is an americium-241 -x-ray source.

Claim 6

Apparatus according to claim 1 wherein the radiation detectors are proportional counters.

Claim 7

Apparatus according to claim 2 wherein the output signal of the first and second detectors are I 1 and I 2 respectively and are expressed by the equations I.sub.1= I.sub.0.sbsb.1 Bexp (-KX.sub.1) and I.sub.2 =I.sub.0.sbsb.2 Bexp (-KX.sub.2) respective where I 0 .sbsb.1 and I 0 .sbsb.2 are values indicative of the values I 1 and I 2 would have if there were no fluid between the source and the first and second radiation detectors, B is a value related to residue build up on the source and on the first and second radiation detectors, K is the linear attenuation coefficient which varies with the density of the fluid, X 1 is the first distance, and X 2 is the second distance and wherein the ratio signal is expressed by the equation ##EQU5## where ΔX is the difference between the first and second distances.

Claim 8

Apparatus according to claim 6 wherein the resultant signal is expressed by the equation ##EQU6## where ρ is the density of the fluid and μ is the mass attenuation coefficient of the fluid.

Claim 9

Apparatus of the class described comprising, in combination: a source of radiation operable to emit radiation generally through a material along a first path; a first radiation detector mounted in the first path at a distance X 1 from the source and operable to produce an output signal I 1 indicative of the radiation received thereby; a second radiation detector mounted in the first path at a distance X 2 from the source and operable to produce an output signal I 2 indicative of the radiation received thereby; and signal receiving means connected to the first and second radiation detectors to receive I 1 and I 2 and to produce a ratio signal which varies with I 1 /I 2 and thus with the density of the material.

Claim 10

Apparatus of the class described comprising, in combination: a source of radiation operable to emit radiation generally through a material along a first path; a first radiation detector mounted in the first path at a distance X 1 from the source and operable to produce an output signal I 1 indicative of the radiation received thereby; a second radiation detector mounted in the first path at a distance X 2 from the source and operable to produce an output signal I 2 indicative of the radiation received thereby; and signal receiving means connected to the first and second radiation detectors to receive I 1 and I 2 and to produce a ratio signal which varies with I 1 /I 2 and thus with the density of the material.

Claim 11

Apparatus according to claim 8 wherein the first and second radiation detectors are of the proportional type.

Claim 12

Apparatus according to claim 9 wherein I 1 =I 0 .sbsb.1 Bexp (-KX 1 ), I 2 =I 0 .sbsb.2 Bexp (-KX 1 ) where K is the linear attenuation coefficient of the material which is equal to the density of the material times the mass attenuation coefficient of the material, B is a value related to the residue build up on the source and the first and second radiation detectors, and I 0 .sbsb.1 and I 0 .sbsb.2 are values indicative of the values I 1 and I 2 would have if there were no material between the source and the first and second radiation detectors.

Claim 13

Apparatus according to claim 10 further including computing means connected to the signal receiving means to receive the ratio signal and operable to produce a resultant signal indicative of the density of the material according to the equation ##EQU7## where ρ is the density of the material, μ is the mass attenuation coefficient of the material and ΔX =X 1 -X 2 .

Claim 14

Apparatus according to claim 11 further including an indicator connected to the signal receiving means to receive the resultant signal.

Claim 15

Apparatus according to claim 12 wherein the source is an americium-241 x-ray source.