fig1 shows a neutron inelastic patient scanning device 100 that is used in accordance with the present invention . a patient 10 lies on the bed 110 . a track 114 , on which the bed 110 rides , is supported by a frame 112 . the bed 110 is propelled on the track by a bed motion control unit 116 to move back and forth in the directions of arrow 12 . near a mid - portion of the track 114 , a shielded high repetition - rate neutron generator 118 is located under the plane of the bed &# 39 ; s motion . two shielded detectors 120 , 122 are placed vertically above the generator 118 on either side of the bed 110 and track 114 to detect the gamma rays from neutron inelastic scattering in the patient . the generator 118 is preferably a sealed , 126 millimeter long tube , which contains an ion source , an accelerator , and a metal tritiated target . a mixture of deuterium and tritium is accelerated at 25 - 60 kev into the target , resulting in the deuterium - tritium fusion reaction . this produces 14 mev neutrons . one such d - t generator is sold by sandia national laboratories . the detectors 120 , 122 are preferably bgo ( bi 4 ge 3 o 12 ) crystal detectors . alternatively , nai ( tl ) detectors may be used . when nai detectors , however , are exposed to thermal neutrons resulting from multi - scattering of the fast neutron beam , the crystals become activated , which affects the data acquisition performance . fig2 is a block diagram illustrating the data acquisition and processing portion 102 of the system . the response of each one of the bgo detectors 120 , 122 is supplied to an amplifier 124 and the amplified signal digitized in two analog - to - digital converters 126 , 128 , which are gated by the neutron pulse . the d - t neutron generator 118 comprises a reservoir 130 of deuterium and tritium , which is accelerated toward the tritiated target 132 by an ion source ring 134 . the reservoir 130 is heated by a reservoir drive circuit 136 and the target is placed at a high electrical potential by the dc voltage supply 138 . a target current monitor 140 and high voltage controller 142 are used to ensure that the nuclear reaction at the target is producing the desire quantity of neutrons . a source drive circuit 144 produces a fast electronic timing signal approximately 1 . 5 microseconds before the leading edge of the generated neutron pulse . this signal passes through a gate / delay 146 to synchronize the analog - to - digital converters 126 , 128 so that two gamma - ray spectra are collected for each detector . as a result , the analog - to - digital converters 126 , 128 are triggered to detect the gamma - rays simultaneously within a 10 - 20 microsecond long neutron pulse . the digital data from the analog - to - digital converters 126 , 128 are passed to a system controlling computer 150 through an interface 148 . the computer additionally receives bed positional information from the bed motion control unit 116 . this allows the computer to correlate instantaneous gamma ray counts to the regions of the patient &# 39 ; s body that are currently being irradiated . fig3 is an exemplary spectra detected from a patient . the identified peaks at 4 . 44 mev and 6 . 13 mev arise from the inelastic scattering of the neutrons off of carbon and oxygen atomic nuclei . according to the following derivation , the ratio of these two peaks in the spectra , indicating the carbon - to - oxygen ratio , is correlated to the percent body fat in the patient . the components of lean body mass are water , protein ( pro ), bone ash ( ba ) and glycogen ( gly ). for the purposes of body composition analysis , glycogen can be derived from protein : neutron activation analysis for the in vivo measurement of total body calcium ( tbca ) and nitrogen ( tbn ) has shown that there is a strong correlation between ba and pro . the body compartments are expressible in terms of body weight ( wt ), water and coeff : where a = water *[ 1 / coeff − 1 ] and represents the portion of lean which is not water . although each of the above assumptions is based on a well developed correlation between portions of lean , when taken together they state a constant partition of lean to its components . the contributing compartments of total body carbon ( tbc ) are fat , protein , glycogen and bone ash . the stoichiometry of each compartment is accounted for to calculate tbc . fat is accurately represented by the stoichiometry c 55 h 102 o 6 . in spite of some variation in the composition of triglycerides , the average stoichiometry of fat is constant , at least in its carbon content of 77 %. according to a classic meat amino acid profile ( c 100 h 159 n 26 o 32 s 0 . 7 ), protein contains 53 . 1 % carbon by weight . glycogen ( c 6 h 10 o 5 ) contains 44 . 4 % carbon . bone ash contains 1 . 73 % carbon . similarly , the contributing compartments to total body oxygen ( tbo ) are water , protein , fat , bone ash and glycogen . taking into account the oxygen content of these compartments : combining equations ( 7 ) and ( 9 ) and using ( 5 ), expression for the ratio of total carbon to total oxygen is derived . c / 0 = 0 . 769 * ( wt - water / coeff ) + 0 . 427 * water * ( 1 / coeff - 1 ) 0 . 888 * water + 0 . 273 * water  ( 1 / coeff - 1 ) + 0 . 112 * ( wt - water / coeff ) c / 0 = 0 . 769 - water wt * ( 0 . 342 coeff + 0 . 427 ) 0 . 112 + water wt * ( 0 . 161 coeff + 0 . 615 ) ( 10 ) equation ( 10 ) describes carbon - oxygen ratio ( c / o ) as a function of the hydration coefficient of lean , coeff , and the total amount of water in the body expressed as a fraction of body weight . from the expression for fat in equation ( 5 ), it is observed that fat / wt = 1 - water wt * 1 coeff ( 11 ) so , for each value of fat content ( fat / wt ), there is a corresponding value of water / wt : water / wt = coeff * ( 1 - fat wt ) ( 12 ) using ( 12 ) equation ( 10 ) becomes : c / o = 0 . 769 - ( 1 - f ) * ( 0 . 342 + 0 . 427 * coeff ) 0 . 112 + ( 1 - f ) * ( 0 . 161 + 0 . 615 * coeff )   or ( 13 ) f = 0 . 273 * c / o + 0 . 427 * coeff + 0 . 615 * coeff * c / o - 0 . 427 0 . 161 * c / o + 0 . 427 * coeff + 0 . 615 * coeff * c / o + 0 . 342 ( 14 ) if a hydration coefficient of lean body mass is assumed or detected to be 0 . 732 , for example , the relationship between fat content and the c / o ratio becomes : f = 0 . 723 * c / o - 0 . 114 0 . 611 * c / o + 0 . 655 ( 15 ) where f is the fat content : fat / wt . this equation describes a non - linear relationship between fat content and c / o ratio for a given hydration coefficient of lean . incidently , the equation ( 14 ) relating percent body fat to the carbon - oxygen ratio and hydration coefficient of lean body mass is relatively insensitive to error in the hydration coefficient . fig4 is a plot of the carbon - oxygen ratio as a function of calculated percent body fat for hydration coefficients of 0 . 720 and 0 . 740 . an error in the hydration coefficient results in a only a few percent deviation in the measure percent body fat . fig5 is a method diagram illustrating the technique for determining percent body fat according to the principles of the present invention . the above derived formula relates the percent body fat to a carbon / oxygen ratio and a level of hydration . while the formula includes contributions from bone ash and glycogen , these two components represent a relatively small part of the total carbon and oxygen in individuals . as a result they can be excluded from the analysis or estimated indirectly without degrading the accuracy in some applications . in step 405 , the level of hydration is determined according to any one of a number of separate approaches . first , the level of hydration can be simply assumed . for most healthy populations , the hydration coefficient for lean body mass is 0 . 732 . such an assumption , however , in many circumstances will not provide the required level of accuracy . as a result , a separate direct hydration measurement can be performed . a number of different techniques may be used . isotope dilution using deuterium , tritium , or h 2 18 o is one possibility . the level of hydration of the lean tissue , however , is also determined by using data in some cases . one of two techniques may be used . first , if the patient is diseased , data concerning the hydration for the diseased population provides a good predictor . for example , levels of hydration tend to be higher in patients with diabetes . population data for other individuals having similar hydration effecting syndromes establish the lean tissue hydration for the patient being tested . secondly , if the hydration of this patient has been previously measured , that direct measurement can be used in place of a contemporaneous measurement . prior to irradiation , the system described with reference to fig1 and 2 is calibrated in step 410 . this should be performed on at least daily basis since changes in atmospheric pressure and aging of the generator 118 can affect operation and thus accuracy . in the preferred embodiment , a substance with a known carbon - oxygen ratio is placed in the detector and the detected carbon - oxygen ratio used to calibrate it . for example , sugar is one possibility . in step 415 , the patient is irradiated with neutrons . for this technique involving neutron inelastic scattering , the neutrons must have sufficient energy to excite the nuclei of carbon and oxygen atoms to their a first energy level . for carbon , this requires neutrons having energy of greater than 4 . 8 mev , and for oxygen , neutrons having an energy greater than 6 . 3 mev are required . in the preferred embodiment , the animal body is irradiated with the neutrons in bursts . during those bursts , the number of generated gamma rays is detected using the bgo detectors 120 , 122 in step 420 . the system processor or computer 150 receives the gamma ray count and energy information from analog to digital converters 126 , 128 . this raw data is then corrected using the information from the calibration step . also during the irradiation , the patient is scanned between the d - t generator 118 and bgo detectors 120 , 122 . this allows the determination of a net or average carbon - oxygen ratio for the entire body of the patient . the system controller 150 , however , also saves the detected gamma rays for regions of the body using the feedback from the bed motion control 116 . as a result , the carbon - oxygen ratio for these regions may be also simultaneously determined . for example , the system controller saves the number of gamma rays detected while scanning the lower leg , thigh , lower abdominal region , mid abdominal region , and chest region separately . in the preferred embodiment , the patient is repeatedly scanned over the neutron source is a oscillatory fashion for approximately 30 minutes . the time period allows sufficient data to be collected while maintaining a low total radiation dose without becoming too onerous for the patient . one advantage associated with the present invention is that it operates based upon the carbon - oxygen ratio . previous attempts based upon total body carbon or total body nitrogen have been more sensitive to the particular operation of the neutron generator and detector since they rely on total counts . as a result , if the detector is operating less efficiently , or if the neutron generator is generating fewer neutrons with the appropriate energies , the accuracy of the measurement will be affected and also require more frequent calibration . in the present invention , a ratio is used that factors out effects of slight aging of the detector and generator . in the final step , the system controller 150 after having received the hydration data , then uses the measured carbon - oxygen ratio to produce a measure of the percent body fat in step 425 . this measure is corrected based upon the information from the calibration and the assumed , or measured level of hydration . moreover , combining the detected neutron counts with the bed position information yields the fat composition for regions of the patient &# 39 ; s body . fig6 is plot of percent body fat as measured by the carbon - oxygen ratio and hydrodensitometry . the demonstrates the accuracy of the inventive technique based on the close agreement the accepted and established hydrodensitometry . while this invention has been particularly shown and described with references to preferred embodiments thereof , it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention as defined by the appended claims . those skilled in the art will recognize or be able to ascertain using no more than routine experimentation , many equivalents to the specific embodiments of the invention described specifically herein . such equivalents are intended to be encompassed in the scope of the claims . for example , the hydration level measurement may be performed at any time , before or after the neutron scan .
a technique for determining percent body fat using neutron inelastic scattering is disclosed . it relies on a correlation between a carbon - oxygen ratio in the body and the percent body fat with corrections made for a level of patient hydration in the lean tissue . the animal body is irradiated with neutrons having sufficient energy to inelastically scatter off carbon and oxygen . the resulting gamma rays are detected and counted , and the level of hydration is measured . the ratio of the detected gamma rays and hydration are then related to a proportion of fat in the animal body . this technique provides accuracy approaching that achieved with hydrodensitometry with only small radiation doses between 5 and 20 millirem , but without any requirements for immersion .