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ARTICLE: A Re-examination of the Acid Titration Behavior of Human Mercaptalbumin: CHANGES IN AMPHOTERIC PROPERTIES ASSOCIATED WITH THE N-F TRANSFORMATION Joseph F. Foster and Patricia Clark J. Biol. Chem. 1962, 237:3163-3170. Find articles, minireviews, Reflections and Classics on similar topics on the JBC Affinity Sites . Alerts: • When this article is cited • When a correction for this article is posted Click here to choose from all of JBC's e-mail alerts This article cites 0 references, 0 of which can be accessed free at http://www.jbc.org/content/237/10/3163.citation.full.html#ref-list-1 Downloaded from http://www.jbc.org/ by guest on December 24, 2014 Access the most updated version of this article at http://www.jbc.org/content/237/10/3163.citation THE JOURNAL OF BIOLOGICAL Vol. 237, No. 10, October Printed CHEMISTRY 1962 in U.S.A. A Re-examination of the Acid Titration Behavior of Human Mercaptalbumin CHANGES IN AMPHOTERIC PROPERTIES ASSOCIATED JOSEPH F. FOSTER AND PATRICIA WITH THE N-F TRANSFORMATION* CLARKE From the Department of Chemistry, Purdue University, Lafayette, Indiana (Received for publication, June 8, 1962) and it is absolutely essential to make correction for such binding in the calculation of 2. Unfortunately, however, data on chloride binding are somewhat limited and uncertain, particularly at low pH. Perhaps the most important objection is raised by the studies of Aoki and Foster (6, 7), which indicate that the isoelectric points calculated at various ionic strengths from the known hydrogen ion binding data and the best available chloride binding data do not agree with those determined by electrophoresis. The discrepancy amounted to as much as 8 to 9 charge units in experiments at 0.1 ionic strength in chloride. Barnett and Bull (11) have confirmed a similar discrepancy with several other proteins. These findings appear to be very important and indicate that either (a) chloride binding data are in serious error, or (5) the effective surface charge is not obtained by simple summation of hydrogen and anion binding data. Barnett and Bull arrived at the second conclusion and suggested that some of the positive charges on the protein are in valleys and are not effective insofar as the surface potential is concerned. In any event, whatever the correct interpretation, the results give cause for concern as to the validity of calculations in which a calculated net charge is employed. An alternative approach was suggested by Hartley and Roe (12)) namely, the experimental evaluation of the surface potential from measurements of electrophoretic mobility and application of the Henry equation. This approach has been utilized by Chattoraj and Bull (13) in a study of the titration behavior of stearic acid and of octadecylamine adsorbed on the surface of Nujol particles. By this appraoch they were able to compute, for the adsorbed acids or bases, effective values of pKi,t that agree well with known values. Beychok and Warner (14) have also utilized this approach in a study of the titration behavior of a protein, lysozyme. A detailed study of the electrophoretic behavior of human mercaptalbumin in acid solution has been reported (15). In the present study, the titration curve of this protein has been redetermined with the same protein preparation and the same experimental conditions as those employed in the electrophoretic studies. The combined data on hydrogen ion binding, electrophoretic mobility, and N-F composition as a function of pH have been subjected to extensive analysis. The results show clearly that the titration anomaly is associated primarily with the N-F reaction and not with expansion. In addition, the results suggest that the isomerization leads to an unmasking or normalization of a large number of carboxylate groups, possibly as many as 50, that are essentially masked in the native form. 3163 Downloaded from http://www.jbc.org/ by guest on December 24, 2014 It is now well known that the titration curves of the plasma albumins, both human and bovine, cannot be fitted satisfactorily The through the classical Linderstrom-Lang titration equation. observed anomaly is an abnormal steepening of the binding curve near the midpoint of the carboxyl titration region, i.e. near pH 4. This anomaly was first pointed out by Tanford (I), who suggested that the abnormality is due to expansion of the protein molecule with consequent reduction of the electrostatic interaction parameter, w. In the years since this suggestion was made, the reversible expansion of albumin at pH below 4 has been well established (2-5). Now, it is also well established, however, that the expansion is preceded by another important transformation, the N-F transformation, which does not involve any important increase in the hydrodynamic volume of the protein but does lead to other important changes in properties (5). It was pointed out by Aoki and Foster (6, 7) that the major part of the anomaly in the titration curve is in all probability associated The with the N-F transformation rather than with expansion. most compelling argument for this hypothesis is the fact that most of the anomaly occurs in the pH range 4.5 to 4.0, a range in which essentially no expansion occurs but in which isomerization does take place. It was shown that to a reasonable approximation the titration curve of bovine plasma albumin could be explained on the basis that in the native or N form all of the carboxy1 groups are abnormal with pKi,t of approximately 3.7, whereas in the isomerized or F form they are essentially normal 4.4). Loeb and Scheraga (8) have also (PKint, approximately concluded that the titration anomaly cannot be explained in terms of expansion and have suggested certain hydrogen-bonded structures that might explain the observed results. All such arguments are somewhat tenuous, however, in that they are based on application of the Debye-Hiickel theory, which assumes the protein to be a rigid, spherical molecule with homogeneous distribution of charges on the surface. Elaborations of the theory that include various assumed positionings of charges have been considered by Tanford and Kirkwood (9). Perhaps an even more pertinent objection is the uncertainty as to the precise net charge, 2. It is well known that the albumins have an unusual propensity to bind anions, even chloride ions (10) * This paper, taken from the Ph.D. thesis of Patricia Clark (Purdue University, 1962), was presented in part before the First International Congress of Biophysics, Stockholm, August 1961. The work was supported by Grant C-2248 of the National Cancer Institute, United States Public Health Service. t Present address, Gerontology Branch, National Institutes of Health, Baltimore City Hospital, Baltimore, Maryland. Amphoteric Properties and N-F Transformation Vol. 237, No. 10 RESULTS FIG. strength obtained (17). 1. Titration curve of human mercaptalbumin, 0.10 ionic (chloride), 0”. Shown for comparison are four points at this same temperature in 0.15 M chloride by Tanford EXPERIMENTAL PROCEDURE Xateriuls-Human mercaptalbumin was prepared from human plasma Fraction V’ through its mercury dimer essentially by the Dintzis method (16). Isoionic solutions of the monomer were prepared by passage of concentrated solutions of the dimer through the thioglycolate and mixed bed ion exchange columns specified by Dintzis. To defat the monomer the pH was lowered to 2.5 or 3.0 for 48 hours and the fatty acid-like material was removed from the turbid solution by centrifugation or filtration. The monomer was tested for the presence of dimer by ultracentrifugal analysis of a 0.8 to 1 y0 solution of the isoionic monomer. Usually about 5% of dimer was present in each stock solution of monomer prepared. An electrophoresis determination with 0.2% protein at pH 4.0 in 0.02 ionic strength chloride was run on each freshly prepared solution of monomer (15). The ratio of the areas of the two peaks was checked against previous data to determine whether the protein had the normal properties. Reagent grade potassium chloride and hydrochloric acid were employed. All water used in the preparation of protein solutions and reagents was distilled and deionized by passage through a demineralizing column.2 1 Obtained through the courtesy of Dr. J. N. Ashworth of the American National Red Cross. We are indebted to Dr. H. Saroff of the National Institutes of Health for suggested modifications of the Dintzis procedure for crystallization of the mercury dimer. 2 Barnstead Bantam, Barnstead Still and Sterilizer Company, Boston, Massachusetts. The titration results, in the usual form of equivalents of hydrogen ions bound plotted against pH and measured relative to the isoionic pH, are shown graphically in Fig. 1. The few previously published experimental data at 0’ on human mercaptalbumin in this pH range, those of Tanford (17), are given for comparison. Tanford’s data were obtained in 0.15 M chloride rather than in 0.1 M, as employed in the present experiments, but otherwise the conditions were probably comparable. The most striking difference is clearly in the isoionic pH, which is 5.78 in the present experiments as compared to Tanford’s 5.17. This difference is doubtless mostly due to the fact that in the much earlier experiments the protein preparations were deionized by electrodialysis rather than by the Dintzis column. Dintzis (16) has reported an isoionic pH of 5.72 for human mercaptalbumin at 2.5” and 0.1 M KCl. It will be noted that the increment in bound hydrogen ions over the range covered by Tanford’s data is almost exactly the same as ours over the same pH range. In Table I are collated the data employed in the calculations to be summarized in the “Discussion.” Since titration and electrophoretic data were not obtained at the same pH values, the data employed were obtained only from smoothed curves of the titration, mobility, and N-F composition data. As a consequence, the calculated points in all cases formed smooth curves, and it was not necessary to include them in subsequent graphs. DISCUSSION Theory-The standard free energy of ionization of a proton from a particular acid site on a protein depends on both the intrinsic standard free energy change and on the over-all change in free energy resulting from the change in charge on the macromolecule. Thus formally 3 Type Al534 supplied byMicrochemica1 California. Specialties, Berkeley 3, Downloaded from http://www.jbc.org/ by guest on December 24, 2014 Preparationof SolutionsAll solutions of protein were prepared from the concentrated isoionic stock solutions previously mentioned. The protein solutions were diluted to 0.98% protein in 0.10 N potassium chloride before titration with 0.104 N hydrochloric acid. The hydrochloric acid solution was standardized against 0.0832 N potassium hydroxide that had previoulsy been standardized with dried potassium acid phthalate. Titration Xtudies-The titration studies \yere carried out on the B or expanded scale of a Beckman Model GS pH meter with a glass electrode and a silver-silver chloride reference electrode with ground glass junction. Fisher standard buffer, pH 4.00, was used to standardize the pH meter at the beginning and end of the titration. The concentration of the protein solutions was measured in a Beckman model DU spectrophotometer; E:& was assumed to be 5.30 at 280 rnp. Once the protein solution had been prepared with the proper amount of potassium chloride, it and the tips of the electrodes were chilled in an ice bath before the titration was started. The titration was performed by the continuous method with a microburette3 that was calibrated just before the titration studies were begun. Total dilution of the protein solution at the lowest pH did not exceed 15%. Blank corrections were determined and applied in the usual fashion whenever they were significant. The calculations of equivalents of hydrogen ions bound per mole were based on an assumed molecular weight of 69,000. October J. F. Foster and P. Clark 1962 AF” = AFiat If $J is the surface potential and E the elementary charge on the proton, it follows that (dF)/(dZ) = Neti. Also remembering that AZ is -1 for loss of a proton, 0 AF” = AFi,t - NC* (2) In terms of ionization constants K and Kint and the corresponding values of pK, equivalent forms of Equation 2 are K = Kinter+lkT (3a) and pK = pKi,t Assuming n equivalent - 0.434&kT (3b) sites, v of which are protonated, pK = pH - log-- n--u ” TABLE (1) + = PKint - 0.434.$/kT (4) 22 $ = - (l/b - ~/l + Ka) D (5) where D is the dielectric constant. As was pointed out in the introduction, this treatment demands knowledge of 2, a parameter that is in fact very uncertain. Hartley and Roe (12) pointed out that the surface potential, #, can be approximated through measurement of the electrophoretic mobility, EL,and use of the Henry equation. The Henry equation (19) strictly yields a “{ potential,” the potential at an imaginary surface of shear that must be somewhat outside the true surface of the molecule. Assuming the difference between the { and the true surface potential to be negligible, the potential is given by Here 77 is the solvent viscosity in poise. The limitations and merits of this treatment have been discussed adequately by Chattoraj and Bull (13) and by Beychek and Warner (14) and need not be further elaborated here. It is worth re-emphasizing, however, that Equation 6 makes minimal demands on knowledge of the size and shape of the protein. For a sphere, the radius a enters only through I, which is a slowly varying function of a. Although the equation is strictly applicable only to spherical molecules, mathematical relationships have been suggested (19) for relating the mobility of a cylinder to that of an equivalent sphere. Aoki and Foster (6, 7) utilized these relationships and concluded that the mobility of bovine plasma albumin with an assumed axial ratio of 4: 1 should be equivalent to that of a spherical molecule with a radius 100/67 times that of the effective radius of the molecule considered as a sphere. Thus, many considerations lead to an estimate of about 30 A for the radius of the plasma albumin molecule, whereas correction of the mobility for the nonspherical shape would lead to an estimate of about 45 A for the effective radius to be employed in Equation 6. At 0.1 ionic strength, the corresponding I values are I Smoothed data employed in calculations PH p x UFl 5.68 5.60 5.47 5.31 5.17 5.00 4.80 4.70 4.60 4.50 4.40 4.30 4.20 4.10 4.00 3.90 3.80 3.70 3.60 3.50 3.10 i 0.7 1.5 2.9 5.1 7.2 10.5 15.0 18.0 21.0 24.5 28.5 33.5 39.0 45.5 51.5 57.0 62.0 67.0 72.0 76.5 91.5 Fraction Ft lo- _- --4.73 -4.53 -4.36 -4.06 -3.77 -3.35 -2.75 -2.40 -1.90 -1.20 -0.15 +0.65 1.55 2.65 3.60 4.45 5.20 5.95 6.65 7.40 7.85 i -0.601 -0.576 -0.555 -0.516 -0.480 -0.426 -0.350 -0.305 -0.242 -0.153 -0.019 +0.083 0.197 0.337 0.458 0.566 0.661 0.756 0.845 0.940 0.997 0.549 0.563 0.575 0.598 0.620 0.654 0.705 0.738 0.786 0.859 0.981 1.09 1.23 1.40 1.58 1.76 1.93 2.13 2.33 2.56 2.71 0 0 0 0 0 0 0 0 0 0 0.03 0.08 0.17 0.41 0.59 0.68 0.77 0.86 0.94 1.00 1.00 *h is the average of ascending and descending mobilities, weighted for composition in cases where both N and F boundaries appear (14). t e)/kT = 1.27 X lo4 /.L. $ N-F Composition (14). 1.10 and 1.13, and there is a difference of only about 3% in the calculated potential. Throughout the calculations that follow a radius of 30 A has been assumed. The factor employed for converting mobility in centigrade-gram-second units to the dimensionless parameter qb/kT, namely, 6 qc/DkTf(Ka), was taken as 1.27 X lo4 for the conditions of the experiments. Before proceeding with the mathematical analysis of the data, it is essential to make some assumption about the state of protonation of the protein at the isoionic pH, the reference pH in these studies. Tanford, Swanson, and Shore (20) have concluded that the imidazolium groups of bovine plasma albumin (16 or 17 in number) have a reasonably normal pKi,t of 6.9. It is assumed that this is also the case for human mercaptalbumin, from which it follows, with due consideration for the electrostatic term, which is substantial at the isoionic pH, that less than 1.0 imidazole group per molecule is unprotonated in the reference state. This assumption has been made, and a small correction has been applied to the observed u values to allow for protonation of imidazole sites. (The correction ranges from -0.2 at pH 5.68 to -0.9 at pH 4.7 and below.) It is assumed that all of the remaining protons are taken up by carboxylate sites. If this is so, and if approximately 100 carboxylate groups are assumed, it can be calculated that approximately three such sites must be protonated at the isoionic pH. The actual number of sites, however, depends upon the interpretation given to the titration curve, as will be considered below. In all of the calculations to be reported it has been assumed that 3.4 carboxylates are protonated at the isoionic pH; this number seems most reasonable on the basis of the various interpretations of the binding cu.rve Downloaded from http://www.jbc.org/ by guest on December 24, 2014 In the usual Linderstrem-Lang (18) treatment, the surface potential is evaluated according to the Debye-Hiickel theory, which assumes the protein molecule to be a sphere with radius b and radius of exclusion a, through 3165 Amphoteric Properties and N-F Transformation 3166 FIG. 2. Plot parameter, -1.40. parison. The of pK = pH - The 0.434 qb/kT. region of the N-F E V/kT log %I-!! versus slope :f the transformation the electrostatic initial dashed line is is shown for com- PH for two extreme models of the FIG. 3. Results of calculations carboxvlate sites in the native human mercantalbumin molecule. Curve a, equivalent abnormal site model, showing effective pKi,t as function of pH (left-hand ordinate). Curve b, masked site model, showing number of titratable sites as function of pH (right-hand ordinate). The region of the N-F transformation is shown for comparison. For further explanation of calculations, see the text. 10 (see below). Only in the case of Fig. 5 and the associated discussion is this assumed number critical, and in that case calculations have been repeated for other assumed states of protonation at the reference pH. In all other cases the graphs and conclusions would not be materially altered by any reasonable change from the number 3.4. Plot of pK against Potential-A standard method of treating protein titration data for the purpose of evaluation of pKi,t has been to plot pK, i.e. (pH - log (n - u)/u), against the electrostatic potential. Usually when the Linderstrom-Lang treatment is followed, such a plot has the calculated charge Z as abscissa; then pKi,t is obtained from the intercept at Z = 0, and the electrostatic interaction parameter w, from the slope (20). In the present case, the appropriate plot by Equation 4 is of pH log (n - LJ)/LJ versus 0.434 qb/kT. In this case, assuming all groups equivalent, a straight line of slope - 1.00 is to be expected, provided that the use of the $J obtained from electrophoretic mobility is in fact justified. In Fig. 2, the data are plotted in this fashion. The most striking result is the flatness of the curve in the region of the N-F transformation. Since in this region there is relatively little expansion, it does not seem reasonable that there should be any essential alteration in the constant that relates # and electrophoretic mobility. The only reasonable interpretation is that this flatness is an artifact of the cooperative transition, and it follows that the slope in this region has no physical signijicance. This being so, it also follows that the parameter w, which would be obtained from the conventional plot in this range, can have no real significance. It can also be concluded that the procedure of obtaining pKi,t by extrapolation to zero potential (charge) cannot yield a meaningful value in this case. Thus, if the curve is extrapolated from the low pH side, a pKi,t of approximately 4.02 is obtained, whereas if extrapolation is made from the high pH side, the value is only 3.90. The slope of the initial linear portion of the curve is -1.40, not -1.00, as theory would predict. At first thought this discrepancy might be taken as indicative of a deficiency in the method of evaluation of the potential #. However, as will be seen below, the effective number of titratable groups in the native form of the protein is probably much less than the 105 assumed in this calculation. If that is the case, the function plotted and the slope obtained can have no physical significance. It is found, in fact, that if n is taken as 55 instead of 105,4 the curve is again linear and of slope very close to - 1.0 down to pH 4.8. This suggests the possibility that, to a first approximation, almost half of the carboxylate sites may be effectively masked in the N form. Calculation of pKcnt as Function of pH, Assuming All Sites EqGvaZent-This is the type of calculation performed by Aoki and Foster (6, 7), who concluded that the mean value of pKi,t changes from approximately 3.7 for the N form to approximately 4.4 for F. In Fig. 3 (Curve a) are shown results of similar calculations made when 105 binding sites, all equivalent, were assumed. In substantial agreement with the previous calculations, which were based on the Debye-Htickel equation and are hence 4 The any type limiting ford (17) molecular indicates, number 107. value 105 was used here because of the fact that almost of analysis applied to our titration data suggests a binding of 100 to 110 protons at extreme acid pH. Tanfound a binding limit of 100 based on the same assumed weight of 69,000 that we have employed. As Fig, 1 approximately 7 protons would have to be added to his to correct for the error in isoionic pH, giving a limit of Downloaded from http://www.jbc.org/ by guest on December 24, 2014 0.434 Vol. 237, No. October 1962 J. F. Foster and P. Clark & = k (n - u) (7) In the presentcasethe electrostaticinteraction canbe introduced through Equation 3a, which yields u eryC/kT = tH+l Thus the appropriate plot is (v/H+)e”‘LT versusu. Such a plot I I 1 I I I I , I IOO- n -4.0 f , I, 0 Fraction I 0.5 I I I I, 1.0 F Form FIG. 4. Plot of the sameparametersas those in Fig. 3 versus the fraction of the F form as obtained from electrophoresis Curve a, equivalent abnormal site model (right-hand ordinate) Curveb, maskedsite model (left-handor&nate). shouldyield a straight line of slope- 1/Ki,t and intercept on the abscissaequal to n, provided that all groupsare equivalent and do not changetheir propertiesthroughout the titration, and provided, of course, that the electrostatic parameter is correctly determined. In the caseof nonequivalent sites, a progressive decreasein slope is expected; i.e. the curve will be monotonic and concave upwards with no inflections. The procedure for handling suchcurves in the caseof nonequivalent siteshas been discussed by Scatchard, Coleman,and Shen (10). In Fig. 5 are shown examplesof Scatchard plots for human mercaptalbuminbasedon three different assumptionsregarding the state of protonation of carboxylate groupsat the isoionicpH. The full curve is basedon the assumptionmadein all previous calculations,namely, that there are 3.4 protonated carboxyls at the isoionicpoint. Consideringonly this curve for the moment, the initial portion, from pH 5.7 to 4.6, is strongly suggestiveof the presenceof some55 equivalent sites of reasonably normal pKi,t (4.3), the rest of the sites being effectively masked (pKi,t

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