Effect of pH buffer molecules on the light-induced currents from oriented purple membrane

• Published in: Biophysical journal 1991-07, Vol.60 (1), p.204-216
• Main Authors: Liu, S.Y., Kono, M., Ebrey, T.G.
• Format: Article
• Language: English
• Subjects: bacteriorhodopsin; Bacteriorhodopsins - physiology; Bacteriorhodopsins - radiation effects; Biological and medical sciences; Buffers; Cell physiology; effects on; Fundamental and applied biological sciences. Psychology; Halobacterium; Halobacterium - metabolism; Hydrogen-Ion Concentration; Kinetics; Light; Molecular and cellular biology; purple membranes; Structure-Activity Relationship
• ISSN: 0006-3495; 1542-0086
• DOI: 10.1016/S0006-3495(91)82044-6

The effect of pH buffers on the microsecond photocurrent component, B2, of oriented purple membranes has been studied. We found that under low salt conditions (less than 10 mM monovalent cationic salt) pH buffers can dramatically alter the waveform of the B2 component. The effect is induced by the protonation process of the buffer molecules by protons expelled from the membrane. These effects can be classified according to the charge transition upon protonation of the buffer. Buffers that carry two positive charges in their protonated form add a negative current component (N component) to B2. Almost all of the other buffers add a positive current component (P component) to B2, which is essentially a mirror image of the N component. Buffers with a pK less than 5.5 have only a small positive buffer component. The pH dependence of the buffer effect is closely related to the pK of the buffer; it requires that the buffer be in its unprotonated form. The rise time of the buffer component increases with the concentration of the buffer molecules. All the buffer effects can be inhibited by the addition of 5 mM of a divalent cation such as Ca2+. Reducing the surface potential slows down the N component but accelerates the P component without affecting the amplitude of the buffer effect significantly. Many of the buffer effects can be explained if we assume that upon protonation of the buffer by a proton expelled from the membrane by light, the buffer molecules move toward the membrane. This backward movement of buffer molecules forms a counter current very similar to that due to cations discussed in Liu, S. Y., R. Govindjee, and T. G. Ebrey. (1990. Biophys. J. 57:951–963).