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A STUDY OF THE EFFECTS OF TIME, BUFFER COMPOSITION, SPECIFIC IONS, AND IONIC STRENGTH ON THE SURFACE TENSION OF SOLUTIONS BETA-LACTOGLOBULIN PDF

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Preview A STUDY OF THE EFFECTS OF TIME, BUFFER COMPOSITION, SPECIFIC IONS, AND IONIC STRENGTH ON THE SURFACE TENSION OF SOLUTIONS BETA-LACTOGLOBULIN

The Pennsylvania State College The Graduate School Department of Agricultural and Biological Chemistry A STUDY OP THE EFFECTS OF TIME, BUFFER COMPOSITION, SPECIFIC I OHS, AND I01TIC STRENGTH OH THE SURFACE TENSION OF SOLUTIONS OF @-LACTOGLOBULIN A Thesis *y Gertrude Haspeslagh Spremulli Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy August, 1942 Approveds (L^j. //__» 1942 ^ Professor of Biophysical Chemistry .-<1 L / ? » 1942 Assistant Professor of Agricultural and Biological Chemistry 2 1942 ,G Hea.d of Department of Agricultural and Biological Chemistry i. TABLE OF CONTENTS Page LIST OF FIGURES - - - - - - - - - - - - - - iii LIST OF TABLES - - - - - - - - - - - - - - v ACKNOWLEDGEMENTS ~ ~ - ----- T± I. INTRODUCTION - - 1 II. REVIEW OF LITERATURE A. Effect of Proteins on Surface Tension and. Its Variation with the pH of the System - - - - - - - - - - - - - - - £ B. Change in Surface Tension of Protein Solutions with Time - - - - - - - - 8 G„ Effects of Buffer Composition, and Ionic Strength on the Property Measured - - - - - - - - - - - - - - l6 D* Resume^ - -- -- -- -- -- -- -- 18 III. THE PROBLEM - -- -- -- - .............- 20 IV. EXPERIMENTAL PROCEDURE A. Preparation of the f^-Lactoglobulin 21 B. Preparation of Stock Solutions of Protein - - - - - - - - - - - - - - 26 Co Preparation of the Buffer Solutions - - - - - - - - - - - - - 27 D0 Surface Tension Meastxrements - - - 28 , V. EXPERIMENTAL RESULTS A. Change of Surface Tension with Time - - - - - - - - - - - - - - - 35 ii TABLE OE CONTENTS (CONTINUED) Page B* Effect of pH on Surface Tension. ^3 C0 Effect of Buffer Composition and of Ionic Strength on Sfurface Tension - - - - - - - - - - - - - 62 D« Comparison of the Surface Tension of Solutions of the Two Crystalline Forms of /^-Lacto- globulin - - - - - - - - - - - - 68 E* Effect of ^-Lactoglobulin Concentration on Surface Tension Lowering - -- -- -- -- -- - 71 VI* DISCUSSION QE RESULTS A* Introductory - - - - - - - - - - 75 B* Influence of Time on Surface Tension Values - - - - - - - - - 78 G* Variation of the Surface Tension with pH - - - - - - - - - - - - 92 D* Effects of Ionic Strength, and Buffer Composition on Surface Tension of Solutions of @ -Lactoglobulin - - - - - - - 102 E« Difference, in Surface Tension of Solutions of the Two Crystalline Eorms of ^-Lactoglobulin - - - 112 E, Conclusion - - - - - - - - - - - 113 VII* SUMMARY -- - - - - - - - - 115 VIII* BIBLIOGRAPHY --- 119 iii LIST OF FIGURES Figure Page globulin a. Tetragonal - - - - - - - - - - 24 b* Tetragonal with Polarized Light - - - - - - - - - - - - 24 c * Grthorhombic - - - - - - - - - 25 2. Change of Surface Tension with Time 36 3« Variation of Log Surface Tension, with Log Time - - - - - - - - - - - - - - - 38 4. Change of Surface Tension Lowering with Time 42 5* Variation of (r* (from equation 1, = <*- + P log t) with pH T a. Sodium Acetate Buffers of Ionic Strength Equal to 0*02 - - 44 b* Sodium Acetate Buffers of Ionic Strength Equal to 0.06 - - 45 c. Sodium Acetate Buffers of Ionic Strength Equal to 0.10 - - 46 d* Magnesium Acetate Buffers of ? Ionic Strength Equal to 0.02 - - 4 e. Magnesium Acetate Buffers of Ionic Strength Equal to 0*06 - - 48 f* Magnesium Acetate Buffers of Ionic Strength Equal to 0.10 - ~ 4-9 60 Relation Between Surface Tension and l/Time - - - - - - - - - - - - - - 50 ?• Effect of Flaslc Aging on Surface Tension - - - - - - - - - - - - - - - 54 8* Effect of pH on Surface Tension Lowering a* Sodium Acetate Buffers of Ionic Strength Equal to 0.02 - - 56 b« Sodium Acetate Buffers of Ionic Strength Equal to 0„06 - - 57 c* Sodium Acetate Buffers of Ionic Strength Equal to 0.10 - - 58 iv LIST OF FIGURES (COHTIHUED) Figure Page d* Magnesium Acetate Buffers of Ionic Strength Equal to 0*02 ——* 59 e* Magnesium Acetate Buffers of Ionic Strength. Equal to 0*06 - ~ 60 f * Magnesium Acetate Buffers of Ionic Strength Equal to 0*10 - - 6l 9« Influence of Buffer Composition on Surface Tension Lowering 64 10. Influence of Ionic Strength on Surface Tension Lowering - -- -- -- -- -- -- 65" 11* Relation Between Ionic Strength and the Minimum in the Surface Tension Lowering- pH Curve - - - - - - - - - - - - - - - - - 66 12* Relation Between Ionic Strength and the Maximum (Acid) in the Surface Tension Lowering-pH Curve - - - - - - - - - - - - 67 13* Variation of h (from log = a - h log t) with. pH - -- -- -- -- -- -- -- -- 70 14« Effect of -Lactoglobulin Concentration on Surface Tension Lowering - - - - - - - - 72 15* Variation of Surface Tension Lowering with Log Log Concentration of # -Lacto- globulin - - - - - - - - - - - - - - - - - 74 LIST OF TABLES Table 1* Values of the Constants a and h To Be Used in the Equation V = ^ , for 0*1 Per Cent Solutions • of -Lac to globulin (Ortho rhomb ic Crystals) - 2* Effect of Flask Aging on the Surface Tension of 0*1 Per Cent Solutions of P -Lactoglobulin (Orthorhombic Crystals) ~ - 3* Values for Surface Tension Lowerings in 0*1 Per Cent Solutions of -Lactoglobulin at Low pH Values - 4* Comparison of Results from the Study ojA Both Crystalline Forms of r -Lactoglobulin in Sodium Acetate Buffers of Ionic Strength Equal to 0.1 » * - - - - - ~ - - - - AC KNO WLED GEME1TT S writer gratefully acknowledges her . , ^ sb to Professor M. W. Lisse for suggesting indebtedn^ and for his advice and heir throughout the probl^ _ ^-fTessor A, H, Palmer for his suggestions and and to Pr<7 , .--ularly in the preparation of the ^-lacto- aid parti<? J * * Both gave valuable assistance during the globulin* jr the manuscript* writing o£ . 1 I. I33TRODUCTIOH The importance of proteins in all phases of "biological chemistry and particularly their importance as components of living matter has made the study of their physical and chemical properties of the greatest interest. Adequate knowledge of their "behavior is., essential to an understanding of the chemistry of life. Ideally, of course, they should he studied under the same conditions as those existing in vivo. Since as yet no entirely satisfactory methods are available for accomplishing this, the alternative is to study them in systems which may be completely characterised in terms of known variables, with the hope that eventually the number and nature of the variables can be made to approach very closely those present in the living cell. That the physical properties of proteins vary with variation in the hydrogen ion concentration (H^O*) of their environment was early noted (Ostwald, 190? {^5T) • This is to be ejected from the fact that proteins are amphoteric electrolytes, existing in solution as" dipolar ions with a net charge which is positive, negative, or zero, depending upon the pH of the medium surrounding them. This variation of physical properties with pH is . 2 so marked that for many years the tendency has heen to explain or interpret the physical behavior of a protein entirely on the basis of the pH of the system* In spite of the fact that the specific effects of added electrolytes have long been recognized, the influence of these same ions when part of a buffer system used to obtain a definite pH lias generally been ignored, and the pH values alone have been used to define the system. Inevitably there has come, especially in recent years, a recognition of the important part played by these ions, other than the hydrogen or hydroxyl, which have had to be introduced into the system in order to create the measured pH, As a result of the important part played by these other ions it is necessary, in order to completely characterize a protein system, to know not only the pH but also the nature and concentration (activity) of the ions introduced to produce that pH* The work reported here was designed to show 7/hether or not the value of an e:cperirnentally determined physical property of a protein is a function only of the pH of the buffer system or whether the specific components of the buffer and its ionic strength also play a part in determining the value of the measured property. Most of the early studies on the physical properties of proteins, such as viscosity, swelling, osmotic pressure, etc*, have shown that they vary in a well-defined, and fairly consistent manner with variation in the pH of the system (39) • generally found that the value of the property was a minimum at the isoelectric point of the protein* A review of the literature revealed, however, that there is a lack of agreement with regard to the variation of the surface tension of a protein solution with pH and that no attention has "been paid to the specific effects of the ions used to obtain the pH. Hence, it was decided that it would he of value to use surface tension as the physical property to he studied. Furthermore, it was felt that knowledge of surface tension values would he of importance from many theoretical points of view - adsorption phenomena, orientation and reaction at interfaces, foaming properties and others. Since it was believed that much of the work on the stirface tension of protein solutions was invalidated by the fact that the proteins used were not pure or homogeneous substances, a protein which would avoid that difficulty ms sought* All data at present indicate that the crystalline lactoglobulin C ^ -lactoglobulin (iiQ.

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