One of the most pervasive weight loss rules is that a cumulative energy deficit of 3500 kcal is required per pound of body weight loss, or equivalently 32.2 MJ kg−1. Under what conditions is it appropriate to use this rule of thumb and what are the factors that determine the cumulative energy deficit required per unit weight loss? Here, I examine this question using a modification of the classic Forbes equation that predicts the composition of weight loss as a function of the initial body fat and magnitude of weight loss. The resulting model predicts that a larger cumulative energy deficit is required per unit weight loss for people with greater initial body fat—a prediction supported by published weight loss data from obese and lean subjects. This may also explain why men can lose more weight than women for a given energy deficit since women typically have more body fat than men of similar body weight. Furthermore, additional weight loss is predicted to be associated with a lower average cumulative energy deficit since a greater proportion of the weight loss is predicted to result from loss of lean body mass, which has a relatively low energy density in comparison with body fat. The rule of thumb approximately matches the predicted energy density of lost weight in obese subjects with an initial body fat above 30 kg but overestimates the cumulative energy deficit required per unit weight loss for people with lower initial body fat.
One of the most pervasive weight loss rules states that a cumulative energy deficit of 3500 kcal is required to lose 1 pound of body weight, or equivalently 32.2 MJ kg−1. The origin of this rule can be traced back to a calculation that assumes exclusive loss of adipose tissue consisting of 87% fat.1, 2 However, Forbes3, 4 has pointed out that lean body mass is lost in concert with body fat during weight loss and it is now generally acknowledged that this rule of thumb is an oversimplification.1 But under what conditions is this rule of thumb appropriate? In other words, what are the factors that determine the cumulative energy deficit required per unit weight loss?
When energy intake does not meet energy requirements, the deficit is accounted for by metabolism of stored energy in the form of body fat, protein and glycogen. Since energy is conserved, the metabolizable energy content of the lost tissue is equivalent to the energy deficit required to produce that weight loss. The metabolizable energy density of the lost tissue is therefore determined by its chemical composition. Loss of body water results in a significant mass change, but contributes nothing to the metabolizable energy content. In contrast, the metabolizable energy densities of body glycogen, protein and fat are 17.6, 19.7 and 39.5 MJ kg−1, respectively.5
Recently, I developed a modification of the classic Forbes equation3, 4 predicting the proportion of weight loss accounted for by loss of lean body mass as a nonlinear function of both the initial body fat as well as the magnitude of weight loss.6 On the basis of this equation, the energy density of weight loss can be predicted once the metabolizable energy densities for the lean body mass loss, ΔL, and body fat mass loss, ΔF, have been determined.
The energy density of the body fat mass change, ρF=39.5 MJ kg−1 is the same as the energy density of fat. It is important to note that the change of body fat, ΔF, is not equivalent to the loss of adipose tissue, which includes a variable contribution of fluid and protein in addition to triglyceride.7, 8 Rather, ΔF is the amount of endogenous fat metabolized by the body to meet the energy deficit. Similarly, the energy density of the lean body mass change, ρL, is determined by the metabolism of tissue glycogen and protein as well as the loss of body water associated with their storage in body tissues. Note that ρL should not be identified with the energy density of the lean body mass as a whole, but rather the energy density of the change of lean body mass. These values are not equivalent. For example, extracellular fluid constitutes a significant fraction of the lean body mass, has a very low energy density, and changes relatively little with weight loss.9, 10, 11, 12 Therefore, ρL has a higher value than the energy density of the lean body mass as a whole.
Both glycogen and protein have similar energy densities and are associated with similar amounts of water in the body tissues.13, 14 However, since glycogen constitutes such a small fraction of the lean body mass and its effects on weight loss typically occur within the first week, ρL is assumed to be derived exclusively from body protein changes and the associated water.2 The water content of the weight change is therefore determined by a protein hydration coefficient, h, which specifies the amount of water lost per gram of body protein change. It has been common to assume that the protein hydration coefficient is equivalent to the total body water divided by the body protein content resulting in a value of about h=3.8 g H2O per gram protein and a value of ρL=4 MJ kg−1. This assumption significantly overestimates the water changes associated with body protein changes since there is a relative increase of lean tissue hydration following weight loss.10 A somewhat better calculation would be the intracellular water divided by the intracellular protein content, resulting in a value of about h=2.8 g H2O per gram protein and a value for ρL=5.6 MJ kg−1. But this calculation also overestimates the protein hydration coefficient because it associates all of the intracellular water with cellular protein while we know that intracellular potassium, as well as other solutes, contributes to determining cellular water content. I propose that h=1.6 g H2O per gram protein is a reasonable estimate for the protein hydration coefficient because this value is in the middle of the range 1.1–2.2 g H2O per gram measured as the osmotically unresponsive water compartment in a variety of cells15 and corresponds to the monolayer hydration of a typical protein.16 This results in a calculated energy density for lean body mass changes of ρL=7.6 MJ kg−1.
Using ρL=7.6 MJ kg−1 and ρF=39.5 MJ kg−1 the energy density of weight loss is simply determined by the relative proportion of lost body weight resulting from lean body mass loss as described by Hall.6 The resulting equation for the metabolizable energy density of the weight loss is: The proportion of the lost weight from lean body mass loss was given by: where Fi is the initial body fat and W is the Lambert W function.6, 17 The factor 10.4 arises from the parameterization of the best-fit logarithmic function used by Forbes to relate lean body mass to body fat mass in a cross-sectional data set of 166 women of similar stature.3, 4, 6
Figure 1a shows the predicted energy density of weight loss as a function of initial body fat mass for weight losses of 5, 25 and 35 kg. The higher the initial body fat, the greater the required cumulative energy deficit required to produce the same amount of weight loss. Greater weight loss is associated with a lower average cumulative energy deficit. These curves are relatively insensitive to exact value of ρL, and the sensitivity decreases for increasing initial body fat (not shown). For example, a 15 kg weight loss for a person with an initial body fat of 20 kg gives a predicted energy density of 24.7 MJ kg−1 weight loss using the recommended h=1.6 g H2O per gram protein and this estimate decreases by only 6.5% to 23.1 MJ kg−1 when using the value h=3.8 g H2O per gram protein.
For comparison, Figure 1a plots the calculated weight loss energy densities from several published weight loss studies. The group averages for each of seven bariatric surgery studies whose obese subjects lost an average of 40.5 kg (▴) are plotted.11, 18, 19, 20, 21, 22, 23 Figure 1a also plots the group averages for four non-surgical weight loss studies whose obese subjects lost an average of 12.5 kg (Δ).24, 25, 26, 27 Since these data cluster around the curves predicted by the modified Forbes equation and the horizontal line in Figure 1, both the modified Forbes equation and the simple 32.2 MJ kg−1 rule of thumb approximate the data reasonably well for obese subjects.
However, the modified Forbes equation predicts deviations from the rule of thumb for weight loss in subjects with relatively low initial body fat. Figure 1a plots the data from individual subjects studied by Keys et al.9 whose lean male subjects lost an average of 16 kg after 6 months of semi-starvation (□). Also plotted are the group average data from three studies of lean subjects28, 29, 30 where the average weight loss was 8 kg (▪). These data indicate that the energy density of weight loss in people with less than 25 kg of initial body fat is indeed significantly lower than the 32.2 kJ kg−1 rule of thumb and approximately conforms to the predicted energy density of the modified Forbes model.
Since it is not common to measure initial body fat in a clinical setting, Figure 1b depicts the curves as a function of initial body weight for the women originally studied by Forbes.3, 4 Since men typically have a higher lean body mass than women for the same amount of body fat, they would be better represented by a rightward shift of the curves in Figure 1b. This rightward shift for men may explain the sexual dimorphism observed in the energy content of weight change for men and women of similar initial body weight.31 In other words, since women typically have more body fat than men of similar body weight, this may explain why men tend to lose more weight than women for a given energy deficit.
The cumulative energy deficit required per unit weight loss is a statement about the metabolizable energy density of the lost body weight, but does not address how such an energy deficit is achieved or maintained. In particular, it is not appropriate to use Figure 1 to calculate the reduction of daily dietary energy required to lose a desired amount of weight over a prescribed period. The following is an example of such an inappropriate calculation: a 163 cm tall woman weighing 65 kg with 20 kg of body fat wants to lose 5 kg of body weight over 6 months. Using Figure 1, she determines that the cumulative energy deficit is 28 MJ kg−1 for a total energy deficit of 140 MJ over 6 months. Therefore, she cuts her energy intake by 780 kJ per day and maintains this diet. Such a calculation fails to account for how an individual's energy expenditure adapts to the energy deficit and decreasing body weight and she will therefore not reach her weight loss goal. The magnitude of the expected energy expenditure adaptation during weight loss is a much debated issue32, 33, 34, 35, 36 and has not been addressed in the present study.
The modification of the classic Forbes equation3, 4 predicts that a sustained energy deficit should result in an increasing rate of weight loss since an increasing proportion of the tissue loss will come from the relatively less energy dense lean body mass.6 The fact that weight loss typically slows over time for a prescribed constant diet9, 37 suggests that either the energy expenditure decreases with time, or the dietary intervention is relaxed over time, or both.
While the present study illustrates that the initial body fat as well as the magnitude of weight loss may influence the applicability of the simple 32.2 MJ kg−1 rule of thumb, it is likely that other factors play a role in the energy density of weight loss beyond what is accounted for by the modified Forbes model. For example, resistance exercise or high protein diets may modify the proportion of weight loss resulting from body fat versus lean tissue.38, 39, 40 A more comprehensive model of macronutrient metabolism and body composition change would be required to model such factors.41
This work was supported by the Intramural Research Program of the NIH, NIDDK.
About this article
Genetic variation in the obesity gene FTO is not associated with decreased fat oxidation: the NEO study
International Journal of Obesity (2017)