A useful measure of an individual's physical condition is the fraction of his or ner body that consist of fat. This problem describes a simple technique for estimating this fraction by weighing the individual twice, once in air and once submerged in water. a. A man has body mass mb = 122.5 kg. If he stands on a scale calibrated to read in newtons, what would the reading be? If he then stands on a scale while he is totally submerged in water at 30 °C (specific gravity = 0.996) and the scale reads 44.0 N, what is the volume of his body (liters)? What is his body density, po (kg/L)? b. Suppose the body is divided into fat and nonfat components, and that xf (kilograms of fat/kilogram of total body mass) is the fraction of the total body mass that is fat: Xf = Mp Prove that 1 1 Pb Xf Pnf 1 1 Ps Pnf Where Pp, Pr, and pns are the average densities of the whole body, the fat component, and the nonfat component, respectively.
A useful measure of an individual's physical condition is the fraction of his or ner body that consist of fat. This problem describes a simple technique for estimating this fraction by weighing the individual twice, once in air and once submerged in water. a. A man has body mass mb = 122.5 kg. If he stands on a scale calibrated to read in newtons, what would the reading be? If he then stands on a scale while he is totally submerged in water at 30 °C (specific gravity = 0.996) and the scale reads 44.0 N, what is the volume of his body (liters)? What is his body density, po (kg/L)? b. Suppose the body is divided into fat and nonfat components, and that xf (kilograms of fat/kilogram of total body mass) is the fraction of the total body mass that is fat: Xf = Mp Prove that 1 1 Pb Xf Pnf 1 1 Ps Pnf Where Pp, Pr, and pns are the average densities of the whole body, the fat component, and the nonfat component, respectively.
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