Hydrostatic weighing: Difference between revisions
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{{Short description|Technique for measuring the density of a living person's body}} |
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{{refimprove|date=June 2011}} |
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'''Hydrostatic weighing''', also referred to as |
'''Hydrostatic weighing''', also referred to as '''underwater weighing''', '''hydrostatic body composition analysis''' and '''hydrodensitometry''', is a technique for measuring the [[density]] of a living person's body. It is a direct application of [[Archimedes' principle]], that an object displaces its own volume of water. |
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==Method== |
==Method== |
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The procedure, pioneered by [[Albert R. Behnke|Behnke]], Feen and Welham as means to later quantify the relation between specific gravity and the fat content,<ref>{{cite journal | doi = 10.1002/j.1550-8528.1995.tb00152.x | journal = JAMA (Reprinted in Obesity Research) | year = 1942 | author1 = Behnke AR | author2 = Feen BG | author3 = Welham WC | pages = 495–498 | volume = 118 | title = The Specific Gravity of Healthy Men| issue = 3 | pmid = 7627779 }}</ref> is based on [[Archimedes' principle]], which states that: |
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The procedure is based on [[Archimedes' principle]], which states that: |
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''The buoyant force which water exerts on an immersed object is equal to the weight of water that the object displaces.'' |
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Example 1: If a block of solid stone weighs 3 kilograms on dry land and 2 kilogram when immersed in a tub of water, then it has displaced 1 kilogram of water. Since 1 liter of water weighs 1 kilogram (at 4° |
Example 1: If a block of solid stone weighs 3 kilograms on dry land and 2 kilogram when immersed in a tub of water, then it has displaced 1 kilogram of water. Since 1 liter of water weighs 1 kilogram (at 4 °C), it follows that the volume of the block is 1 liter and the density (mass/volume) of the stone is 3 kilograms/liter. |
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Example 2: Consider a larger block of the same stone material as in Example 1 but with a 1 |
Example 2: Consider a larger block of the same stone material as in Example 1 but with a 1-liter cavity inside of the same amount of stone. The block would still weigh 3 kilograms on dry land (ignoring the weight of air in the cavity) but it would now displace 2 liters of water so its immersed weight would be only 1 kilogram (at 4 °C). |
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In either of the examples above, the correct density can be calculated by the following equation: |
In either of the examples above, the correct density can be calculated by the following equation:<ref>{{cite book |last1=McArdle |first1=William D |last2=Katch |first2=Frank I |last3=Katch |first3=Victor L |title=Exercise Physiology: Energy, Nutrition, and Human Performance|publisher=Lippincott Williams & Wilkins |year=2010 |isbn=978-0-7817-4990-9 | page = 741|edition=7th }}</ref> |
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:<math> |
:<math>D_b = \frac{M_a}{\frac{M_a - M_w}{D_w} - RV} </math> |
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Where: |
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*{{mvar|D{{sub|b}}}} = Density of the body; |
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*{{mvar|M{{sub|a}}}} = "Mass in air" (i.e. dry weight); |
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*{{mvar|M{{sub|w}}}} = "Mass in water" (i.e. underwater weight); |
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*{{mvar|D{{sub|w}}}} = Density of water (based on water temperature); |
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⚫ | |||
The [[residual volume]] in the lungs can add error if not measured directly or estimated accurately. [[Residual volume]] can be measured by gas dilution procedures or estimated from a person's age and height: |
The [[Lung volumes|residual volume]] in the lungs can add error if not measured directly or estimated accurately. [[Lung volumes|Residual volume]] can be measured by gas dilution procedures or estimated from a person's age and height:<ref>{{cite journal | author = Quanjer P.H., Ed. | title = Standardized Lung Function Testing | publisher = European Community for Coal and Steel, Luxembourg | year = 1983 | journal = Bulletin Européen de Physiopathologie Respiratoire | volume = 19 | issue = suppl. 5 | pages = 1–95}}</ref> |
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* RV-Est(liters, Men) = 1.310 × Ht. (meters) + 0.022 × Age (yrs., take as 25 for 18-25) − 1.232 |
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* RV-Est(liters, Women) = 1.812 × Ht. (meters) + 0.016 × Age (yrs., take as 25 for 18-25) − 2.003 |
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⚫ | These estimates are for adults aged 18-70, have standard deviation of about 0.4 litres and have dependence on ethnicity, environmental factors, etc.<ref>{{cite journal | journal = European Respiratory Journal | year = 1993 | title = Lung volumes and forced ventilatory flows | doi = 10.1183/09041950.005s1693 | volume = 6 | pages = 5–40 | author1 = Ph.H Quanjer | author2 = G.J. Tammeling | author3 = J.E. Cotes | author4= O.F. Pedersen | author5= R. Peslin | author6= J-C. Yernault| issue = suppl. 16 }}</ref> [[Lung volumes|Residual volume]] may also be estimated as a proportion of [[vital capacity]] (0.24 for men and 0.28 for women).<ref>{{cite journal | author = Wilmore, J. H. | title = The use of actual predicted and constant residual volumes in the assessment of body composition by underwater weighing | journal = Med Sci Sports | year = 1969 | volume = 1 | issue = 2 | pages = 87–90 | doi=10.1249/00005768-196906000-00006| doi-access = free }}</ref> |
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Inches: RV-Est(Women) = 0.046 X Ht. (inches) + 0.016 X Age (yrs.) - 2.003 |
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Metric: RV-Est(Women) = 1.812 X Ht. (meters) + 0.016 X Age (yrs.) - 2.003 |
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⚫ | [[Residual volume]] may also be estimated as a proportion of [[vital capacity]] (0.24 for men and 0.28 for women).<ref>{{cite journal | author = Wilmore, J. H. | title = The use of actual predicted and constant residual volumes in the assessment of body composition by underwater weighing | journal = Med Sci Sports | year = 1969 | volume = 1 | pages = 87–90 | doi=10.1249/00005768-196906000-00006}}</ref> |
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==Application== |
==Application== |
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Once body density has been calculated from the data obtained by hydrostatic/underwater weighing, [[body composition]] can be estimated. The most commonly used equations for estimating the percent of body fat from density are those of Siri<ref name="siri">{{citation | author = Siri, SE | chapter = Body composition from fluid spaces and density: analysis of methods | |
Once body density has been calculated from the data obtained by hydrostatic/underwater weighing, [[body composition]] can be estimated. The most commonly used equations for estimating the percent of body fat from density are those of Siri<ref name="siri">{{citation | author = Siri, SE | chapter = Body composition from fluid spaces and density: analysis of methods |veditors= Brozek J, Henschel A | title = Techniques for measuring body composition | location = Washington, DC | publisher = [[United States National Academy of Sciences|National Academy of Sciences]], [[United States National Research Council|National Research Council]] | year = 1961 | pages = 223–34 }}</ref> and Brozek et al.:<ref name="brozek">{{citation | vauthors = Brozek J, Grande F, Anderson JT, Keys A | title = Densitometric Analysis of Body Composition: Revision of some Quantitative Assumptions | journal = Ann. N. Y. Acad. Sci. | volume = 110 | pages = 113–40 | date = September 1963 | issue = 1 | pmid = 14062375 | doi = 10.1111/j.1749-6632.1963.tb17079.x | bibcode = 1963NYASA.110..113B | s2cid = 2191337 }}</ref> |
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Siri (1956): Fat % = [4.950 /Density - 4.500]×100 |
Siri (1956): Fat % = [4.950 /Density - 4.500]×100 |
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*[[Body composition]] |
*[[Body composition]] |
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*[[Composition of the human body]] |
*[[Composition of the human body]] |
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*[[Body fat percentage]] |
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{{DEFAULTSORT:Hydrostatic Weighing}} |
{{DEFAULTSORT:Hydrostatic Weighing}} |
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[[Category: |
[[Category:Anthropometry]] |
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[[Category:Classification of obesity]] |
Latest revision as of 21:40, 4 December 2024
Hydrostatic weighing, also referred to as underwater weighing, hydrostatic body composition analysis and hydrodensitometry, is a technique for measuring the density of a living person's body. It is a direct application of Archimedes' principle, that an object displaces its own volume of water.
Method
[edit]The procedure, pioneered by Behnke, Feen and Welham as means to later quantify the relation between specific gravity and the fat content,[1] is based on Archimedes' principle, which states that: The buoyant force which water exerts on an immersed object is equal to the weight of water that the object displaces.
Example 1: If a block of solid stone weighs 3 kilograms on dry land and 2 kilogram when immersed in a tub of water, then it has displaced 1 kilogram of water. Since 1 liter of water weighs 1 kilogram (at 4 °C), it follows that the volume of the block is 1 liter and the density (mass/volume) of the stone is 3 kilograms/liter.
Example 2: Consider a larger block of the same stone material as in Example 1 but with a 1-liter cavity inside of the same amount of stone. The block would still weigh 3 kilograms on dry land (ignoring the weight of air in the cavity) but it would now displace 2 liters of water so its immersed weight would be only 1 kilogram (at 4 °C).
In either of the examples above, the correct density can be calculated by the following equation:[2]
Where:
- Db = Density of the body;
- Ma = "Mass in air" (i.e. dry weight);
- Mw = "Mass in water" (i.e. underwater weight);
- Dw = Density of water (based on water temperature);
- RV = Residual volume (the unfilled space enclosed by the body- e.g. volume of air in the lungs + respiratory passages after a maximum exhalation).
The residual volume in the lungs can add error if not measured directly or estimated accurately. Residual volume can be measured by gas dilution procedures or estimated from a person's age and height:[3]
- RV-Est(liters, Men) = 1.310 × Ht. (meters) + 0.022 × Age (yrs., take as 25 for 18-25) − 1.232
- RV-Est(liters, Women) = 1.812 × Ht. (meters) + 0.016 × Age (yrs., take as 25 for 18-25) − 2.003
These estimates are for adults aged 18-70, have standard deviation of about 0.4 litres and have dependence on ethnicity, environmental factors, etc.[4] Residual volume may also be estimated as a proportion of vital capacity (0.24 for men and 0.28 for women).[5]
Application
[edit]Once body density has been calculated from the data obtained by hydrostatic/underwater weighing, body composition can be estimated. The most commonly used equations for estimating the percent of body fat from density are those of Siri[6] and Brozek et al.:[7]
Siri (1956): Fat % = [4.950 /Density - 4.500]×100
Brozek et al. (1963): Fat % = [4.570 /Density - 4.142]×100
References
[edit]- ^ Behnke AR; Feen BG; Welham WC (1942). "The Specific Gravity of Healthy Men". JAMA (Reprinted in Obesity Research). 118 (3): 495–498. doi:10.1002/j.1550-8528.1995.tb00152.x. PMID 7627779.
- ^ McArdle, William D; Katch, Frank I; Katch, Victor L (2010). Exercise Physiology: Energy, Nutrition, and Human Performance (7th ed.). Lippincott Williams & Wilkins. p. 741. ISBN 978-0-7817-4990-9.
- ^ Quanjer P.H., Ed. (1983). "Standardized Lung Function Testing". Bulletin Européen de Physiopathologie Respiratoire. 19 (suppl. 5). European Community for Coal and Steel, Luxembourg: 1–95.
- ^ Ph.H Quanjer; G.J. Tammeling; J.E. Cotes; O.F. Pedersen; R. Peslin; J-C. Yernault (1993). "Lung volumes and forced ventilatory flows". European Respiratory Journal. 6 (suppl. 16): 5–40. doi:10.1183/09041950.005s1693.
- ^ Wilmore, J. H. (1969). "The use of actual predicted and constant residual volumes in the assessment of body composition by underwater weighing". Med Sci Sports. 1 (2): 87–90. doi:10.1249/00005768-196906000-00006.
- ^ Siri, SE (1961), "Body composition from fluid spaces and density: analysis of methods", in Brozek J, Henschel A (eds.), Techniques for measuring body composition, Washington, DC: National Academy of Sciences, National Research Council, pp. 223–34
- ^ Brozek J, Grande F, Anderson JT, Keys A (September 1963), "Densitometric Analysis of Body Composition: Revision of some Quantitative Assumptions", Ann. N. Y. Acad. Sci., 110 (1): 113–40, Bibcode:1963NYASA.110..113B, doi:10.1111/j.1749-6632.1963.tb17079.x, PMID 14062375, S2CID 2191337