J Appl Physiol 95: 620-630, 2003.
First published March 28, 2003; doi:10.1152/japplphysiol.00100.2003
8750-7587/03 $5.00
Experimental determination of net protein charge and Atot and Ka of nonvolatile buffers in human plasma
Henry R. Staempfli1 and
Peter D. Constable2
1Department of Clinical Studies, Ontario
Veterinary College, University of Guelph, Guelph, Ontario, Canada N1G 2W1; and
2Department of Veterinary Clinical Medicine, College
of Veterinary Medicine, University of Illinois, Urbana, Illinois 61802
Submitted 31 January 2003
; accepted in final form 26 March 2003
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ABSTRACT
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The mechanism for an acid-base disturbance can be determined by using the
strong ion approach, which requires species-specific values for the total
concentration of plasma nonvolatile buffers (Atot) and the
effective dissociation constant for plasma weak acids
(Ka). The aim of this study was to experimentally
determine Atot and Ka values for human plasma
by using in vitro CO2 tonometry. Plasma PCO2
was systematically varied from 25 to 145 Torr at 37°C, thereby altering
plasma pH over the physiological range of 6.907.55, and plasma pH,
PCO2, and concentrations of quantitatively important
strong ions (Na+, K+, Ca2+, Mg2+,
Cl-, lactate) and buffer ions (total protein, albumin, phosphate)
were measured. Strong ion difference was estimated, and nonlinear regression
was used to calculate Atot and Ka from the
measured pH and PCO2 and estimated strong ion
difference; the Atot and Ka values were then
validated by using a published data set (Figge J, Rossing TH, and Fencl V,
J Lab Clin Med 117: 453467, 1991). The values (mean ±
SD) were as follows: Atot = 17.2 ± 3.5 mmol/l (equivalent to
0.224 mmol/g of protein or 0.378 mmol/g of albumin); Ka =
0.80 ± 0.60 x 10-7; negative log of
Ka = 7.10. Mean estimates were obtained for strong ion
difference (37 meq/l) and net protein charge (13+.0 meq/l). The experimentally
determined values for Atot, Ka, and net protein
charge should facilitate the diagnosis and treatment of acid-base disturbances
in critically ill humans.
plasma pH; strong ion difference; anion gap; metabolic acidosis
THE STRONG ION APPROACH TO acid-base balance emphasizes that the
pH and bicarbonate concentration ([HCO3]) of an aqueous biological
solution are determined by three independent variables (for review, see Refs.
4,
5,
36): 1)
PCO2; 2) strong ion difference (SID), which is
the difference between the charge of strong cations (sodium, potassium,
calcium, magnesium) and strong anions (chloride, lactate, sulfate, ketoacids,
nonesterified fatty acids, and many others) that are completely dissociated in
biological solutions; and 3) the total weak acid concentration
(Atot), which includes all nonvolatile weak acids in the system,
such as proteins and inorganic phosphates that are modeled as having a single
effective dissociation constant (Ka). The physicochemical
interactions between the independent and dependent variables in an acid-base
system recognize the constraints imposed by the law of electrical neutrality,
the dissociation equilibrium of weak acids, and the conservation of mass
(4,
36). The strong ion approach
can be used to determine the contribution of the three independent variables
(PCO2, SID, Atot) to plasma pH and
[HCO3], thereby improving our understanding of physiological and
pathophysiological interactions in biological aqueous solutions.
Plasma proteins provide the major contribution to Atot, and,
therefore, plasma protein concentration independently affects acid-base
balance. The role of plasma protein concentration in acid-base balance is well
recognized in human and veterinary medicine, with hypoproteinemia and
hyperproteinemia causing alkalemia and acidemia, respectively
(5,
11,
20,
29). The most widely used
method to assign a value for Atot in human plasma has been
calculation from the plasma protein concentration by using the estimate of net
protein charge obtained by Van Slyke and colleagues
(39) in 1928. To obtain this
estimate, human plasma proteins were assumed to have the same alkali titration
curve as horse serum proteins
(40); this assumption provided
an estimate for the net protein charge of human plasma ([total protein] = 70
g/l, where brackets denote concentration) of 16.9 meq/l. In a 1964 study, Van
Leewen (38) estimated that the
net protein charge in human plasma was 12.6 meq/l, a value that was similar to
the estimate of 12.0 meq/l obtained by Figge and colleagues
(10) in 1992. Many
investigators assumed that these estimated values for net protein charge
(16.9, 12.6, or 12.0 meq/l) were equivalent to the value for Atot;
however, this is an erroneous assumption, because the value for
Atot must always be greater than that of net protein charge, and
because Atot is expressed in different units (mmol/l) than net
protein charge (meq/l) (6).
Species-specific values for Atot and Ka
should be experimentally determined when using the strong ion approach to
describe acid-base equilibria
(4,
35,
36). Values for
Atot (14.9 or 15.0 mmol/l) and Ka (2.1 or 2.2
x 10-7) have been experimentally determined for equine plasma
(4,
35), but different values have
been experimentally determined for cattle plasma (Atot = 25.0
mmol/l; Ka = 0.9 x 10-7; Ref.
7) and cat plasma
(Atot = 27.4 mmol/l; Ka = 1.0 x
10-7; Ref. 21). For
human plasma, only theoretical estimates for Atot (24.1 mmol/l) and
Ka (1.1 x 10-7) are available
(6). Interestingly, these
theoretical Atot and Ka estimates predicted
that net protein charge in human plasma was 15.3 meq/l, which was similar to
the estimate of Van Slyke et al. (16.9 meq/l)
(39), but greater than that of
Van Leeuwen (12.6 meq/l) (38)
and Figge et al. (12.0 meq/l)
(11). The purpose of this
study was, therefore, to experimentally determine Atot and
Ka values for human plasma and, from this information,
calculate net protein charge. We accomplished our objectives by performing in
vitro CO2 tonometry of plasma from eight healthy humans. We also
validated the experimentally determined values for Atot and
Ka using published data
(11) and compared the
predictive accuracy of these values with theoretical estimates
(6) or derived estimates
(10,
32).
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MATERIALS AND METHODS
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Blood and plasma collection. Twenty milliliters of venous blood
were collected into lithium-heparin tubes from the antecubital veins of eight
healthy humans (2646 yr old; 4 men, 4 women). Lithium-heparin tubes
were used instead of sodium-heparin tubes for blood collection, because the
measured sodium component of plasma collected into sodium-heparin can be
increased by up to 2 meq/l, increasing the measured SID
(44). In addition,
lithium-heparin dissociates in plasma into a strong cation (lithium) and
strong anion (sulfite), with no change in actual SID or measured SID, because
plasma lithium and heparin concentrations are not routinely measured.
One milliliter of venous blood was immediately analyzed to characterize the
normal values, and plasma was harvested from the remaining 19 ml by
centrifugation that was completed within 30 min of collection. Plasma was
frozen at -70°C and stored for up to 2 mo before being thawed at room
temperature immediately before CO2 tonometry was performed. The
University of Guelph ethics committee approved this study.
CO2 tonometry of plasma. Plasma
samples were tonometered (IL 235, Instrumentation Laboratory, Lexington, MA)
for 20 min at 37°C over a PCO2 range of 25145
Torr by using a gas mixture containing 20% CO2 and 80% normal air.
This produced a pH range of 6.907.55.
Blood and plasma analyses. The fresh blood sample and all
tonometered plasma samples were analyzed in duplicate on a Statprofile 9+
(NOVA Biomedical, Canada, Mississauga, Ontario) for blood-plasma gas analysis
(pH, PCO2) and determination of [Na+],
[K+], [Ca2+], [Cl-], and
[lactate-]. Table 1
provides a summary of the variability and measurement methodology for each
variable. An untonometered plasma sample was analyzed in duplicate (Dacos
multianalyzer, Coulter Electronics, Hialeah, FL) to determine strong cation
(Mg2+) and nonvolatile buffer ion (total protein, albumin, and
inorganic phosphate) concentrations.
Calculation of SID. Strong cation (Na+ + K+
+ Ca2+ + Mg2+) and strong anion (Cl- +
lactate) concentrations were assumed to be constant during CO2
tonometry and an ionic equivalency assigned to those variables
(Mg2+, lactate) not measured by using ion-selective potentiometry.
Accurate measurements of SID are difficult to obtain in plasma
(6,
31,
42) because of cumulative
measurement error, presence of unknown strong anions
(12,
15), and differences in
equipment and methodology (18,
28); SID was, therefore,
initially estimated by using three methods: SID3 =
{([Na+] + [K+]) - [Cl-]}; SID4 =
{([Na+] + [K+]) - ([Cl-] + [lactate])}; and
SID6 = {([Na+] + [K+] + [Ca2+] +
[Mg2+]) - ([Cl-] + [lactate])}. A constant value for
SID3, SID4, and SID6 was assigned by using
the mean value for all CO2 tonometered samples from each subject.
This minimized the effect of measurement variability in strong ion
concentrations. A constant value for SID is one of the assumptions of the
strong ion approach; SID is invariant over the physiological range of pH,
because strong ions are fully dissociated at physiological pH
(4,
6,
33). Because SID3,
SID4, and SID6 represented constant values, the terms
were expressed as [SID3]constant,
[SID4]constant, and
[SID6]constant, respectively.
In preliminary data analysis, strong ion (Na+, K+,
Ca2+, and Cl-) concentrations measured by ion-selective
electrodes were regressed against pH. Neither [K+] or
[Cl-] varied with pH; however, [Na+] varied inversely
with pH for six of the eight plasma samples (mean linear regression equation:
[Na+] = -3.98 pH + 173.5), and [Ca2+] varied inversely
with pH for all eight plasma samples (mean linear regression equation:
[Ca2+] = -1.29 pH + 11.9), where [Na+] and
[Ca2+] were in meq/l. Over the pH range in this study
(6.907.55), this corresponds to a mean change in [Na+] and
[Ca2+] of 2.6 and 0.8 meq/l, respectively. A possible reason for
the observed pH dependence of measured [Na+] and [Ca2+]
was poor selectivity of the sodium and calcium electrodes to H+.
The potentiometric selectivity coefficient defines the ability of an
ion-selective electrode to distinguish the primary ion from other ions in the
same solution; the smaller the value for the selectivity coefficient, the less
susceptible is the electrode to changes in the concentration of the
interfering ion (3). Although
reported selectivity coefficients of the Ca2+, Na+, and
K+ electrodes for H+ are 0.1616, 0.23.2,
and <0.0001, respectively
(1), these selectivity
coefficient values were not high enough to explain the pH dependency of
[Na+] and [Ca2+] during CO2 tonometry over a
pH range of 6.907.55.
The most likely reason for the pH dependency of measured [Na+]
and [Ca2+] was salt-type binding of sodium and calcium to plasma
protein; as pH decreases, the net protein charge decreases (becomes less
negative), thereby "releasing" electrostatically bound sodium and
calcium and increasing plasma [Na+] and [Ca2+] when
measured by ion-selective potentiometry
(3,
19,
23). As we observed, the
magnitude of this effect was more pronounced for Na+ than
Ca2+, because 36 mmol of sodium and 0.8 mmol of calcium are
electrostatically bound to plasma proteins for each liter of human plasma
(3). To account for the effect
of pH on electrostatically bound sodium and calcium, we calculated the SID for
each tonometered plasma sample from the measured values for [Na+],
[K+], [Ca2+], [Mg2+], [Cl-], and
[lactate] and termed this value [SID6]variable, because
the value varied with pH during CO2 tonometry.
Calculation of Atot and
Ka. Measured values for pH and
PCO2, calculated values for
[SID3]constant, [SID4]constant,
[SID6]constant, and
[SID6]variable, the six-factor simplified strong ion
electroneutrality equation (4)
 | (1) |
and the Marquardt nonlinear regression procedure
(13,
30) were used to solve
simultaneously for Atot and Ka, where
[A-] in Eq. 1 is the net charge of plasma nonvolatile
buffers. To facilitate accurate calculation of values for Atot and
Ka, Eq. 1 was expressed in the following form
 | (2) |
by applying known values for the solubility of CO2 in plasma (S;
0.0307 mmol · l-1 · mmHg-1)
(2) and the negative logarithm
of the apparent equilibrium dissociation constant
(pK'1; 6.120 at [NaCl] = 0.16 mmol/l; interpolated
from Table II, Ref.
14). With the use of the value
of 6.120 for pK'1 calculated actual plasma
[HCO3] (mmol/l) at 37°C
(25); similarly, the four
methods used to calculate SID provided a value in terms of concentration. This
means that Eq. 2 estimated a value for Atot in terms of
concentration (mmol/l). The form of the simplified strong ion
electroneutrality equation used in Eq. 2 was selected because it
provided the narrowest confidence intervals for the estimated values of
Atot and Ka. Initial estimates for
Atot of 530 mmol/l in increments of 5 mmol/l and initial
estimates for Ka of 0.13.0 x 10-7
in increments of 0.1 x 10-7 were used for the nonlinear
regression procedure.
Because the true value for SID was unknown, a fifth nonlinear regression
procedure was performed to simultaneously estimate values for Atot,
Ka, and SID (called [SID]estimated), with
initial estimates for [SID]estimated of 3045 meq/l in
increments of 5 meq/l.
A sixth nonlinear regression procedure was performed to calculate
Atot and Ka. This was done to compare
Atot and Ka values obtained by using the
six-factor simplified strong ion model (described previously) with Stewart's
eight-factor strong ion model
(36). Although we have shown
algebraically (4) and
graphically (6) that Stewart's
eight-factor strong ion model contains two redundant factors [apparent
equilibrium dissociation constant for the ion product of water
(
) and apparent equilibrium
dissociation constant for
],
it was of interest to determine whether the eight-factor model provided more
accurate estimates for Atot and Ka. Measured
values for pH and PCO2, calculated values for
[H+](= 10-pH), either [SID]variable or
[SID]estimated, the carbonate ion concentration
([
]), and the hydroxyl ion
concentration ([OH-]), Stewart's eight-factor strong ion
electroneutrality equation
(36)
 | (3) |
and the Marquardt nonlinear regression procedure
(30) were used to solve
simultaneously for Atot and Ka. To facilitate
the nonlinear regression procedure, Eq. 3 was expressed in the
following form
 | (4) |
Where pK'3 is the negative logarithm (10.22) of the
apparent equilibrium dissociation constant for HCO3
(K'3 = 6 x 10-11) and
pK'w is the negative logarithm (13.36) of the ion
product of water (K'w = 4.4 x
10-14). The form of the strong ion electroneutrality equation used
in Eq. 4 was selected because it provided the narrowest confidence
intervals for the estimated values of Atot and
Ka when pH was changed by CO2 tonometry.
R2 values were calculated for the seven fitted
nonlinear regression models by using the values obtained during CO2
tonometry of each human plasma sample: the six-factor simplified strong ion
model and five different methods ([SID3]constant,
[SID4]constant, [SID6]constant,
[SID6]variable, [SID]estimated) for
estimating SID, and the eight-factor strong ion model and two different
methods ([SID6]variable, [SID]estimated) to
estimate SID. The calculated Atot values were indexed to the total
protein (Atot tp) and albumin (Atot-alb) concentration,
and mean ± SD values for Atot, Atot tp, Atot
alb, and Ka were determined. A P value
<0.05 was considered significant.
Comparison and validation of calculated Atot
and Ka values. Serum electrolyte
concentrations, PCO2, protein concentrations, and pH
values were extracted from a published data set of human serum filtrands with
experimentally induced changes in PCO2, SID (expressed
as concentration), and [total protein] (Ref.
11,
Table 2). These data were used
to compare and validate the mean Atot tp, Atot alb, and
Ka values obtained by using the six-factor simplified
strong ion model and five different methods for assigning a value to SID,
[SID3]constant, [SID4]constant,
[SID6]constant, [SID6]variable,
and [SID]estimated, or the eight-factor strong ion model using
[SID6]variable and [SID]estimated. In
addition, the calculated Atot tp and Ka values
were compared with previous estimates [Atot tp = 0.344 mmol/g of
total protein, Ka = 1.05 x 10-7
(6); Atot tp = 0.340
mmol/g of total protein, Ka = 0.56 x 10-7
(32); Atot tp =
0.334 mmol/g of total protein, Ka = 0.42 x
10-7 (10,
11)]. Calculated Atot
alb values were also compared with previous Atot estimates
derived from the albumin concentration [Atot alb = 0.572 mmol/g of
albumin (6); Atot
alb = 0.553 mmol/g of albumin
(32); Atot alb =
0.545 mmol/g of albumin (10,
11)].
Serum pH was calculated by using the six-factor simplified strong ion
equation (3) in the following
form
 | (5) |
the measured variables PCO2, SID = ([Na+] +
[K+] + [Ca2+] + [Mg2+] - [Cl-] -
1.5), and [total protein]; known values for S (0.0307 mmol ·
l-1 · mmHg-1)
(2) and
pK'1 (6.120)
(14,
25); and the calculated values
for Atot tp, Atot alb, and Ka. The
subtraction of 1.5 from the SID value represented the estimated charge on the
unmeasured strong anion sulfate in the serum filtrand
(11). The calculated pH was
then compared with the measured pH by using linear regression analysis, and
the R2, coefficient, and intercept values were used for
comparison with the line of identity (slope = 1; intercept = 0).
Calculation of net protein charge. The [A-] (in meq/l)
at physiological pH (7.40) was calculated from the experimentally determined
values for Atot and negative log of acidic dissociation constant
(pKa) (8)
as
 | (6) |
The value for [A-] calculated in Eq. 6 represents the net
negative charge of nonvolatile plasma buffers (albumin, globulin, phosphate);
the value for [A-] is, therefore, pH dependent. Protein and
phosphate also have a pH-independent negative charge that acts as a strong
anion charge (41). In albumin
and globulin, this is due to carboxyl, phenolic, and guanidium groups
(37), and on phosphate it is
due to the
moiety.
The pH-dependent component of net phosphate charge
([phosphate-]; in meq/l) at physiological pH (7.40) was calculated
as
 | (7) |
The net protein charge (in meq/l) at physiological pH (7.40) was calculated as
[A-] - [phosphate-]. This calculates the pH-dependent
component of protein charge and not the total protein charge.
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RESULTS
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Blood and plasma analyses. The values for venous blood from eight
humans are presented in Table
2. A total of 157 CO2 tonometered plasma samples were
analyzed, representing 1623 tonometered samples from each human.
Representative PCO2 and pH values obtained during
CO2 tonometry of plasma from two humans are shown in
Fig. 1.
Calculation of SID. For normal plasma, mean values for
[SID3] (40.9 meq/l), [SID4] (40.0 meq/l), and
[SID6] (43.0 meq/l) were obtained
(Table 2). Different mean
values for [SID3]constant (43.8 meq/l) (Tables
3,
4,
5),
[SID4]constant (41.9 meq/l),
[SID6]constant (46.0 meq/l) (Tables
3,
4,
5), and
[SID]estimated (37.1 meq/l) were obtained during tonometry (Tables
6 and
7). The mean range for
[SID6]variable during tonometry was 7.5 meq/l (Tables
8 and
9).
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Table 3. Summary of calculated values for Atot, Atot tp,
Atot alb, and Ka obtained using
[SID3]constant = ([Na+] + [K+]) -
[Cl-]
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Table 4. Summary of calculated values for Atot, Atot tp,
Atot alb, and Ka obtained using
[SID4]constant = ([Na+] + [K+]) -
([Cl-] + [lactate])
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Table 5. Summary of calculated values for Atot, Atot tp,
Atot alb, and Ka obtained using
[SID6]constant = ([Na+] + [K+] +
[Ca2+] + [Mg2+]) - ([Cl-] +
[lactate])
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Table 6. Summary of calculated values for Atot, Atot tp,
Atot alb, Ka, and [A-] (at pH = 7.40)
obtained using [SID]estimated from the 6-factor strong ion
model
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Table 7. Summary of calculated values for Atot, Atot tp,
Atot alb, Ka, and [A-] (at pH = 7.40)
obtained using [SID]estimated from the 8-factor strong ion
model
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Table 8. Summary of calculated values for Atot, Atot tp,
Atot alb, and Ka obtained using
[SID6]variable = ([Na+] + [K+] +
[Ca2+] + [Mg2+]) - ([Cl-] + [lactate]) from
the 6-factor strong ion model
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Table 9. Summary of calculated values for Atot, Atot tp,
Atot alb, and Ka obtained using
[SID6]variable = ([Na+] + [K+] +
[Ca2+] + [Mg2+]) - ([Cl-] + [lactate]) from
the 8-factor strong ion model
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Calculation of Atot and
Ka. The R2 value for all
nonlinear regression models was >0.98, indicating excellent fit to the
data. The calculated values for Atot and Ka
depended markedly on the value assigned to SID (Tables
3,
4,
5,
6,
7,
8,
9;
Fig. 2).

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Fig. 2. Plot of calculated total weak acid concentration value (indexed to total
protein) (Atottp) against estimated value for strong ion difference
(SID). Values are means ± 1 SD. Note that the calculated value for
Atottp depends on the estimated value for SID.
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When pH = 7.40 and PCO2 = 40 Torr, the actual
[HCO3] = 23.4 mmol/l (calculated from the Henderson-Hasselbalch
equation when S = 0.0307 mmol · l-1 ·
mmHg-1 and pK'1 = 6.120). Accordingly,
the true SID of human plasma at pH = 7.40 can be calculated by using the
simplified strong ion electroneutrality equation (Eq. 2) so that SID
= 23.4 + 11.5 = 34.9 meq/l. The calculated value for true SID was within the
95% confidence interval (2945 meq/l) estimated by using nonlinear
regression (Table 6). Applying
the measured values for the mean venous blood values in this study
Table 2; pH = 7.37,
PCO2 = 51 Torr, Atot = 17.2 mmol/l
(calculated from a [total protein] of 76.9 g/l), Ka = 0.80
x 10-7, S = 0.0307 mmol · l-1 ·
mmHg-1, pK'1 = 6.120} to Eq. 5
predicted that SID = 39 meq/l, which was also within the 95% confidence
interval (2945 meq/l) for the calculated SID value.
Comparison and validation of calculated Atot
and Ka values. With the use of a data
set containing 72 serum filtrands from two humans and calculating
Atot from the [total protein], the highest R2
value (0.967) was obtained from the Atot and Ka
estimates obtained with [SID]estimated in the six-factor strong ion
model and Atot indexed to [total protein]
(Table 10). The most accurate
values were, therefore, Atot = 17.2 ± 3.5 mmol/l (equivalent
to 0.224 mmol/g of protein), Ka = 0.80 ± 0.60
x 10-7, and pKa = 7.10. These estimated
values for Atot and Ka were only one of four
pairs of values where the fitted regression line was the same as the line of
identity (slope = 1; intercept = 0); the values for Atot and
Ka obtained by Siggaard-Andersen et al. in 1977
(32) and Constable in 2001
(6) also fitted the line of
identity, but had lower R2 values. In addition, Stewart's
eight-factor strong ion model with [SID]estimated
(Table 10) was very close to
the six-factor strong ion model (R2 = 0.965). The
Atot and Ka values derived by Figge et al. in
1992 (10) from their data set
(11) did not fit the line of
identity.
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Table 10. Summary of calculated mean values for SID, Atottp, and
Ka, and linear regression results for calculated pH (dependent
variable) against measured pH (independent variable)
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With the use of the same data set and calculating Atot from the
albumin concentration, the highest R2 value (0.960) was
obtained from the Atot and Ka value obtained
with [SID]estimated, followed very closely by Stewart's
eight-factor model with [SID]estimated (R2 =
0.959) (Table 11). The
Atot value was equivalent to 0.378 mmol/g of albumin. As before,
the estimated values for Atot and Ka obtained
with [SID]estimated was one of four, where the fitted regression
line was the same as the line of identity; the values for Atot and
Ka obtained by Siggaard-Andersen in 1977
(32) and Constable in 2001
(6) also fitted the line of
identity, but had lower R2 values. The Atot and
Ka values derived by Figge et al. in 1992
(10) from their data set
(11) did not fit the line of
identity.
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Table 11. Summary of calculated mean values for Atot alb and
Ka, and linear regression results for calculated pH (dependent
variable) against measured pH (independent variable)
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Calculation of net protein charge. The [A-] at
physiological pH (7.40) for each tonometered human plasma sample was
calculated from the experimentally determined values for Atot and
pKa obtained by using [SID]estimated:
[A-] = Atot/[1 + 10(
pKa-pH)] = 10.8 ± 4.0 meq/l
(Table 6). This estimate for
[A-] reflected the charge assigned to the pH-dependent components
of albumin, globulin, and phosphate; because the pH-dependent component of
phosphate charge at physiological pH (7.4) was 1.0 meq/l (calculated by using
Eq. 7 and data in Table
2), the mean net protein charge in the eight human plasma samples
attributed to nonvolatile buffer ions was 9.8 ± 4.0 meq/l = 0.215 meq/g
albumin ([albumin] = 45.5 g/l) or 0.127 meq/g total protein ([total protein] =
76.9 g/l).
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DISCUSSION
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In this study, we experimentally determined and validated values for
Atot (17.2 mmol/l) and Ka (0.8 x
10-7) of human plasma. We also found that the values for
Atot and Ka depended markedly on the estimated
value for SID. Determining the true value for SID remains the major difficulty
in applying the strong ion approach to acid-base disturbances.
This appears to be the first study to use nonlinear regression to
simultaneously estimate values for Atot, Ka,
and SID; the values obtained for Atot and Ka at
the same time as SID provided the most accurate prediction of pH from known
values for PCO2, [Na+], [K+],
[Ca2+], [Mg2+], [Cl-], [lactate], and [total
protein] in filtrands of human plasma. This suggests that the true mean SID of
the eight plasma samples was 37 meq/l. This value was lower than that
estimated as [SID3] ([Na+] + [K+] -
[Cl-] = 41 meq/l), [SID4] ([Na+] +
[K+] - [Cl-] - [lactate] = 40 meq/l), and
[SID6] ([Na+] + [K+] + [Ca2+] +
[Mg2+] - [Cl-] - [lactate] = 43 meq/l); less than the
estimated value of 4042 meq/l
(15,
16,
17,
33); but similar to the value
calculated by Watson in 1999
(41) (38 meq/l). Clearly,
unidentified strong anions are present in human plasma. These unidentified
strong anions include sulfate, D-lactate, nonesterified fatty
acids, and ketoacids; however, concentrations of these anions are too low to
explain all of the unmeasured anion charge.
We believe that unaccounted protein and phosphate charge are responsible
for most of the unmeasured strong anion charge in human plasma. Protein and
phosphate charge have two components: a fixed charge that functions as a
strong anion [the net difference in charge between carboxyl, epsilon-amino,
phenolic, and guanidium groups in proteins
(41) and
in phosphate], and a variable
charge that functions as a nonvolatile buffer ion (due mainly to imidazole
groups in protein and
and
in phosphate)
(Fig. 3). To quantify the
pH-independent and -dependent components of protein and phosphate charge, the
concentrations of protein and phosphate would need to be varied. When the
effect of variations in protein concentration on pH was investigated in human
plasma, the net anionic charge assigned to albumin at pH = 7.40 has been 0.25
meq/g (9), 0.268 meq/g
(24), 0.27 meq/g
(41), 0.33 meq/g
(20), or 0.408 meq/g
(29). All five estimates for
net anionic charge for albumin were higher than that obtained in this study
(0.215 meq/g albumin at pH = 7.40); however, our estimate reflects only the
pH-dependent (nonvolatile buffer ion) charge of albumin and not the strong ion
charge. Accordingly, the negative charge on albumin should be
compartmentalized into a pH-independent strong ion charge (
0.305 - 0.215
= 0.090 meq/g albumin, where 0.305 is the mean of the 5 estimates for the net
anion charge of albumin and 0.215 is our estimate for the nonvolatile buffer
ion charge of protein, assuming only albumin contributes to protein charge), a
pH-dependent nonvolatile buffer ion charge, which can be calculated from the
known values for pH, phosphate concentration, and the negative logarithm to
the base 10 of the dissociation constant (1.58 x 10-7) of
, and
experimentally determined values for Atot and
Ka. The formula for calculating net protein charge (in
meq/l) from the albumin concentration (in g/l) and the phosphate concentration
(in mmol/l) is, therefore
 | (8) |
where protein charge is indexed to the albumin concentration, and the
pH-dependent component of phosphate charge is subtracted from the assigned
nonvolatile buffer ion charge. At normal values for pH (7.40), [albumin] (41
g/l), and [phosphate] (1.2 mmol/l), Eq. 8 calculates pH-independent
protein charge = 3.7 meq/l, pH-dependent nonvolatile buffer ion charge = 10.3
meq/l, and pH-dependent phosphate charge = 1.0 meq/l; the net protein charge
of human plasma = 3.7 + 10.3 - 1.0 = 13.0 meq/l. This value for net protein
charge was similar to that obtained by Van Leewen in 1964
(38) (12.6 meq/l) and Figge et
al. in 1992 (10) (12.0
meq/l).

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|
Fig. 3. Schematic of the effects of 3 independent variables on pH. Note that
albumin, globulin, and phosphate contribute to both SID and total weak acid
concentration (Atot). NEFAs, nonesterified fatty acids.
|
|
A similar approach can be applied to calculating net protein charge from
the [total protein]. The net anionic charge assigned to total protein in human
plasma has been 0.179 meq/g
(38), 0.243 meq/g
(29), or 0.26 meq/g
(20). These three estimates
for net total protein charge were higher than that obtained in this study
(0.127 meq/g total protein at pH = 7.40); however, as discussed previously,
our estimate reflects only the pH-dependent component and not the
pH-independent (strong anion) component. Of these three estimates, the value
obtained by Van Leewen (0.179 meq/g)
(38) appears to be the most
accurate, as it was developed from a net protein charge of 12.6 meq/l.
Accordingly, protein charge can be compartmentalized into a pH-independent
strong ion charge (
0.179 - 0.127 = 0.052 meq/g total protein, where 0.179
is Van Leewen's estimate and 0.127 is our estimate for the nonvolatile buffer
ion charge of plasma proteins) and a pH-dependent buffer ion charge, which can
be calculated as described previously for albumin (Eq. 8). The
formula for calculating net protein charge (in meq/l) from the [total protein]
(in g/l) and the [phosphate] (in mmol/l) is, therefore
 | (9) |
where protein charge is indexed to the [total protein] and the pH-dependent
component of phosphate charge is subtracted from the assigned nonvolatile
buffer ion charge. At normal values for pH (7.40), [total protein] (70 g/l),
and [phosphate] (1.2 mmol/l), Eq. 9 calculates the net protein charge
of human plasma = 3.6 + 10.4 - 1.0 = 13.0 meq/l. This value for net protein
charge was identical to that obtained from the albumin concentration
alone.
Which method should we use clinically to calculate net protein charge? The
R2 values from linear regression of calculated pH against
measured pH (Tables 10 and
11) indicated that expressing
Atot in terms of [total protein] provided the most accurate fit to
the data.
However, albumin is the most important buffer in plasma (73% of total
buffering), with globulins contributing 22% of total buffering and phosphate
5% of total buffering (32). It
is widely believed that the net protein charge is more accurately calculated
from albumin (9,
20,
24,
29,
41) than total protein
(20,
29,
38), principally because of
individual variations in the albumin-to-globulin ratio. However, the
widespread use of ion-selective electrodes has lowered the reference range of
the anion gap {[Na+] - ([Cl-] +
[
])} for human plasma from
816 meq/l (9,
24) to 311 meq/l
(43), indicating that the
unmeasured anions exceed the
unmeasured cations by 311
meq/l. By attributing charges to quantitatively important anions, protein
(13.0 meq/l when calculated from albumin or total protein in humans with
normal albumin-to-globulin ratios), phosphate (2.2 meq/l), lactate (0.9
meq/l), and quantitatively important cations, potassium (4.2 meq/l), calcium
(2.3 meq/l), and magnesium (1.6 meq/l), the net charge that can be attributed
to the quantitatively important components of the anion gap is 8.0 meq/l.
Because this estimate lies within the range of the normal anion gap
(311 meq/l) for human plasma, net protein charge can be calculated from
either albumin concentration or protein concentration.
Because of difficulties in obtaining the true value for SID, the major
clinical utility in using the strong ion approach in critically ill patients
is to calculate the strong ion gap to detect and quantify the unmeasured
strong cation or anion concentration
(7,
8). Based on the previous
discussion and the results of this study, the two most accurate equations for
calculating strong ion gap (in meq/l) in human plasma are
 | (10) |
and
 | (11) |
where anion gap (in meq/l) = [Na+] - ([Cl-] +
[
]), and [albumin] and [total
protein] are in g/l. Equations 10 and 11 assume that the
unmeasured strong cation concentration (K+, Ca2+,
Mg2+) equals the unmeasured strong anion concentration (lactate,
sulfate, nonesterified fatty acids, ketoacids, pH-independent phosphate
charge, and other strong anions); the strong ion charge of albumin or protein
is included in Eq. 10 or 11. At normal values of pH (7.40),
[albumin] = 41 g/l, and anion gap = 7 meq/l, Eq. 10 calculates the
strong ion gap
-0.4 meq/l. At normal values of pH (7.40), [total protein]
= 70 g/l, and anion gap = 7 meq/l, Eq. 11 calculates the strong ion
gap
-0.2 meq/l. For the venous blood samples from the eight humans in
this study, pH (7.37), [albumin] = 45.5 g/l, anion gap = 6.5 meq/l, Eq.
10 calculates the strong ion gap
0.6 meq/l, and with the use of
[total protein] = 76.9 g/l, Eq. 11 calculates the strong ion gap
0.7 meq/l. These calculations suggest that the strong ion gap equations
(Eqs. 10 and 11) provide a useful method for detecting the
presence and quantifying the magnitude of unmeasured anions in the plasma of
critically ill human patients; presently the unmeasured anions are suspected
to be predominantly associated with uremia
(22,
26).
Finally, which value for SID should be used in the strong ion approach?
Because the mean actual SID (37 meq/l) for the eight plasma samples was
estimated to be 4 meq/l less than [SID3] = ([Na+] +
[K+]) - [Cl-] = 41 meq/l
(Table 2), 3 meq/l less than
[SID4] = ([Na+] + [K+]) - ([Cl-] +
[lactate]) = 40 meq/l, and 6 meq/l less than [SID6] =
([Na+] + [K+] + [Ca2+] + [Mg2+]) -
([Cl-] + [lactate]) = 43 meq/l, and because mean plasma
[K+] = 4 meq/l, we suggest the following equations for calculating
actual SID from measured SID
 | (12) |
 | (13) |
 | (14) |
 | (15) |
Obviously, Eqs. 1215 assume that the
unmeasured anions
equal the
unmeasured cations and that plasma albumin and total protein
concentrations are normal.
 |
DISCLOSURES
|
|---|
This study was supported by EP Taylor Equine trust fund, by Natural
Sciences and Engineering Research Council of Canada, and by Ontario Ministry
of Agriculture, Food and Rural Affairs-Equine Program.
 |
ACKNOWLEDGMENTS
|
|---|
The technical expertise of Dr. Susanne Misiaszek, Bonnie Lambert, and Dr.
Nevil Sukra is greatly appreciated.
 |
FOOTNOTES
|
|---|
Address for reprint requests and other correspondence: H. R. Staempfli, Dept.
of Clinical Studies, Ontario Veterinary College, Univ. of Guelph, Guelph,
Ontario, Canada N1G 2W1 (E-mail:
hstaempf{at}uoguelph.ca).
The costs of publication of this article were defrayed in part by the
payment of page charges. The article must therefore be hereby marked
"advertisement" in accordance with 18 U.S.C. Section 1734
solely to indicate this fact.
 |
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