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- Rosalind S. Gibson
- University of Otago
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Accurate methods for measuring body composition are required in investigations of obesity, malnutrition, weight loss following bariatric surgery, muscle wasting, sarcopenia, osteopenia, and osteoporosis. Body composition information is also used to establish the appropriate prognosis and treatment of hospital patients, and with longitudinal assessment, to monitor the effects of interventions on body composition (Lemos & Gallagher, 2017).
Selection of the method to measure body composition depends on the required precision and accuracy, the study objective, cost, convenience to the subject, their health, and equipment and technical expertise available(Lukaski, 1987). Methods based on multi-component models that include analysis of protein and minerals, minimize assumptions related to tissue density, hydration, and structure. This is important because in malnourished individuals, the elderly, and subjects with metabolic disturbances, the relative proportions of the body components is often altered, and losses of protein, fat, and bone mineral content may occur, often in association with the rapid accumulation of water. Changes such as these invalidate the determination of fat and the fat-free mass in the 2‑component model.
Absolute validity cannot be assessed for any of the indirect in vivo body composition methods because the gold standard for body composition analyses is cadaver analysis. Instead, only relative validity can be assessed, defined as the comparison for each subject of the results from the “test” method with the results from another method, termed the “reference or criterion” method; the latter having a greater degree of demonstrated validity. A 4‑component model is now considered sufficiently accurate to act as a reference or criterion method, but its use in many settings is limited because of the expensive and sophisticated technology required. Multiple statistical approaches can be used to establish the validity of the “test” method compared with a reference method. They include regression and correlation analyses, paired t tests, and more recently, Bland-Altman analysis; see Earthman (2015) for further details.
The characteristics of the various procedures used for measuring body composition are summarized in Box 14.1. This list includes both non-scanning and scanning techniques. Detailed sections (14.2‑14.12) describe each of these indirect in vivo methods now available to assess body composition. Comments on these methods are also given, along with the assumptions used, and the advantages and disadvantages of each method. Scanning techniques such as computer tomography (Section 14.9), magnetic resonance imaging (Section 14.10) and whole body dual energy X‑ray absorptiometry (DXA) (Section 14.11) are included together with a discussion of their clinical importance (Lee et al., 2019; Neeland et al., 2019). Each technique generates body composition data in different ways, so the methods are not interchangeable. Methods with the lowest cost are often the most imprecise.
Methods employing the 2‑component model (i.e., body fat and fat-free mass) include total body potassium, total body water via isotope dilution or bioelectrical impedance, densitometry via hydrostatic weighing or air-displacement plethysmography, and total body electrical conductivity. Such methods are not suitable for clinical populations when the basic assumptions of the 2‑component model are often invalid. Instead, in these populations, techniques using a 3, 4, or 5‑component model should be applied. For example, (Section 14.11) has the capacity to generate data that can be used with a 3‑component model. See Lohman (1986) and Pietrobelli et al. (1996) for further details.
Three scanning techniques — computerized tomography (Section 14.9), magnetic resonance imaging (Section 14.10), and DXA (Section 14.11) — can be used to quantify components (e.g., skeletal muscle, bone, visceral ectopic fat) at the tissue-organ level of body composition as well as to assess the relative proportions of the fat-free mass, body fat, and bone mineral content. Of these, only DXA has been recommended for the assessment of fat mass in patients with a variety of disease states; the use of DXA for the assessment of fat-free mass is not recommended for clinical populations because its validity for assessment of fat-free mass in any clinical population remains unknown (Sheean et al., 2020).
Box 14.1. Scanning and non-scanning laboratory techniques used to measure body composition.
- 14.1 Chemical analysis of cadavers
Cadaver analysis provides the gold standard data on body composition, but the use of such data is limited by ethical barriers. Results from a few older studies (1945‑1968) are mostly based on adults who had died because of illness. - 14.2 Total body potassium (TBK)
TBK is measured by counting radiation from naturally occurring 40K in a whole body counter. Required equipment is only found in specialized facilities. Estimates of the fat-free mass can be derived from the TBK. - 14.3 Total body water from isotope dilution (TBW)
A tracer dose of water, usually labeled with the stable isotope 2H, is given orally or intravenously and then allowed to equilibrate. The concentration of the isotope in serum, urine, or saliva is measured and TBW calculated from dilution observed following equilibration. Obesity, pregnancy, and wasting disease increase TBW. - 14.4 Multiple dilution methods
Typically, multiple dilution involves determining both total body water via isotope dilution and extracellular water (ECW), the latter using a tracer such as bromide that does not enter the intracellular space. The difference between these two measurements (i.e., TBW − ECW) reflects the intracellular water. - 14.5 In vivo activation analysis
Radioactive isotopes of N, P, Na, Cl, Ca are created by irradiating the subject. The resulting γ‑radiation is measured using a whole body counter. Subjects are exposed to radioactivity. Sensitivity varies with the element. Required equipment is only found in specialized facilities. - 14.6 Densitometry
Body density is derived from measurements of body mass and body volume. The latter is calculated from: (a) the apparent loss of weight when the body is totally submerged in water — difficult with young children, the elderly or sick patients — or, (b) air-displacement or water-displacement plethysmography. - 14.7 Total body electrical conductivity (TOBEC)
Subject lies supine in a solenoid coil through which a 5MHz current is passed. The conductivity value of the subject is obtained by subtracting the background value when the coil is empty. Edema, ascites, dehydration, electrolyte balance and variations in bone mass all interfere with the conductivity reading. - 14.8 Bioelectrical impedance (BIA)
The impedance to a weak electrical current passed between the right ankle and right wrist of a subject in supine position is measured. Edema, ascites, and dehydration invalidate single frequency measurements. Multifrequency measurements allow estimation of both total and extracellular compartments. - 14.9 Computerized tomography (CT)
Method measures attenuation of X-rays as they pass through tissues, the degree of attenuation being related to differences in physical density of the tissues. An image is reconstructed from the matrix of picture elements. Exposure to ionizing radiation limits use of CT for pregnant women or children. Expensive equipment. - 14.10 Magnetic resonance imaging (MRI)
Imaging involves placing a subject in a very strong magnetic field and observing the relative differences in behavior of 1H protons in lean and adipose tissue. No exposure to ionizing radiation but equipment bulky and expensive. - 14.11 Dual energy X‑ray absorptiometry (DXA)
Utilizes the attenuation of a dual energy X‑ray beam, often during whole-body scanning. New fan-beam technologies replacing earlier pencil-beam techniques lead to lower X‑ray doses and improved spatial resolution. High precision method, but results are calibration dependent and differences between various equipment manufacturers can be significant. - 14.12 Ultrasound
High-frequency sound waves from a combined ultrasound source and meter pass through adipose tissue to the adipose-muscle tissue interface. At the interface, some sound waves are reflected back as echoes, which are translated into depth readings via a transducer. CT, MRI, or DXA provides higher degree of structure resolution than ultrasound.