Adsorption of single-stranded and double-helical polynucleotides on the mercury electrode

The adsorption of single-stranded polynucleotides and double-helical DNA on the dropping mercury electrode has been studied with the aid of Breyer's alternating current (a.c.) polarography. Our results indicate that all three constituents of polynucleotides (residues of bases, sugar, and phosphoric acid) are involved in the adsorption. At neutral pH their participation in adsorption depends on the ionic strength, the potential of the electrode, and the conformation of the polynucleotide in the solution. At an ionic strength of about 0.1, double-helical DNA is adsorbed electrostatically on a positively charged electrode surface by inadequately masked negative charges of the phosphate groups. At a higher ionic srength (about 0.5), this electrostatic adsorption is no longer detectable by using a.c. polarography; under these conditions it is probable that native DNA is adsorbed around the potential of the electrocapillary maximum with the aid of sugar residues and a few bases. Single-stranded polynucleotides, on the other hand, are primarily adsorbed by means of the bases. Desorption of double-helical DNA occurs around a potential of ?1.2 V against SCE. At this potential, the helical regions of single-stranded polynucleotides are also desorbed. Desorption of the disordered regions of single-stranded polynucleotides occurs at more negative potentials. Adsorption and desorption of a small number of bases released from double-helical DNA was evident in the a.c. polarograms only at elevated temperature, or at room temperature after degradation of DNA by sonication.     

Interaction of nucleic acids with electrically charged surfaces: II. Conformational changes in double-helical polynucleotides

The influence of adsorption of double-stranded (ds) DNA, ds RNA and homopolymeric pairs at a mercury electrode on conformation of these polynucleotides was studied. Changes in the polarographic reducibility of polynucleotides, which were followed by means of normal pulse polarography and linear sweep peak voltammetry at the dropping mercury electrode were exploited to indicate conformational changes. It was found that, as a consequence of adsorption of ds polynucleotides on the negatively charged electrode conformational changes similar to denaturation take place in a narrow potential region around ?1.2 V (the region U). After sufficiently long time of the contact with the electrode (under our conditions about 10 s) these changes reach limiting values, which can approach total denaturation. Upon adsorption of ds polynucleotides on the electrode charged to more positive potentials than the region U either (1) no conformational changes occur or (2) only a small part of the polynucleotide (probably labile regions of the ds molecule) is very quickly denatured - the remainder of the molecule preserves its ds structure. Conformational changes of adsorbed ds polynucleotides are influenced by factors which change the stability of ds polynucleotides in solution. It is supposed that denaturation of ds polynucleotides in the region U might result from the strains connected with the repulsion of certain segments of the molecule anchored on the electrode from the negatively charged surface.     

Über die Adsorption von DNS in der Grenzfläche Quecksilber–Elektrolyt

The adsorption of deoxyribonucleic acid (DNA) in the mercury–electrolyte interface has been investigated. The effect of this adsorption on the differential capacity of the electrical double layer between a polarized mercury surface and an 0.15M NaCl solution containing DNA was measured by means of the alternating current polarography (Breyer polarography). The effective alternating current ? under actual conditions (adsorption processes only, small electrolytic resistance, small alternating current frequency, and alternating current amplitude) is directly proportional to the differential double layer capacity. The combination of this method with the application of a stationary mercury drop electrode allows the coverage of the electrode to be followed, continuously in the range 0.2 sec, to about 60 sec. The diffusion is the rate-controlled step of the adsorption kinetics. Therefore the lowering of the alternating current ? by the adsorbed DNA is proportional to the surface concentration for partly covered surface and reaches a constant value after the surface becomes fully covered. Adsorption of further layers does not affect the differential capacity. This makes it possible to determine the maximum surface concentration of the DNA. For that it is necessary to determine the diffusion coefficient of DNA. This was done directly by Strassburger and Reinert in our institute. The surface concentrations of the native DNA and the relative surface concentrations of the denatured DNA in dependence on the potential of the polarized mercury surface was estimated. Both surface concentrations show a pronounced dependence on the potential with a minimum of the surface concentration around ?0.4 V with respect to the normal calomel electrode. This property may be caused by the structure of the adsorption layer depending on the potential. That means that only several segments at the rigid DNA molecules are adsorbed and the other ones remain in the solution near the surface. The adsorption in the neighborhood of the electrocapillary zero potential at ?0.4 V is strongest, and therefore the fraction of the adsorbed segments has a maximum. At these potentials consequently the maximum coverage is already reached at relatively low surface concentrations. Opposite to this is Miller's hypothesis, that native DNA preserves its double helical structure when adsorbed on a negatively charged mercury surface, whereas unfolding occurs on a positively charged mercury surface. Miller's hypothesis is supported by facts that the surface concentration of the denatured DNA should be independent of the potential and should be equal to the surface concentration of the native DNA at a positively charged mercury surface. But an evaluation of Miller's diagrams by no means gives an independence on the potential of the surface concentration of the denatured DNA and no accordance between the surface concentrations of denatured and of native DNA's at the positively charged mercury surface. Moreover Miller compared different DNA samples with different moleculer weights and possibly with different molecular weight distributions. Both the molecular weight and the molecular weight distribution have a pronounced influence on the surface concentration. Therefore this accordance mentioned above is not evident. The critical inspection of Miller's work and the own investigation lead to the conclusion that an unfolding or denaturation of native DNA does not take place in the mercury–electrolyte interface.     

Nucleotide sequence-dependent opening of double-stranded DNA at an electrically charged surface

It has been shown earlier that the DNA double helix is opened due to a prolonged contact of the DNA molecule with the surface of the mercury electrode. At neutral pH, the opening process is relatively slow (around 100 s), and it is limited to potentials close to -1.2 V (against SCE). The opening of the double helix has been explained by strains in the DNA molecule due to strong repulsion of the negatively charged phosphate residues from the electrode surface where the polynucleotide chain is anchored via hydrophobic bases. Interaction of the synthetic ds polynucleotides with alternating nucleotide sequences/poly(dA-dT).poly (dA-dT), poly (dA-dU).poly (dA-dU), poly (dG-dC).poly (dG-dC)/ and homopolymer pairs/poly (dA).poly (dT), poly (rA).poly (rU) and poly (dG).poly (dC)/ with the hanging mercury drop electrode has been studied. Changes in reducibility of the polynucleotides were exploited to indicate opening of the double helix. A marked difference in the behaviour was observed between polynucleotides with alternating nucleotide sequence and homopolymer pairs: opening of the double-helical structures of the former polynucleotides occurs at a very narrow potential range (less than 100 mV) (region U), while with the homopolymer pairs containing A X T or A X U pairs, the width of this region is comparable to that of natural DNA (greater than 200 mV). In contrast to natural DNA, the region U of homopolymer pairs is composed of two distinct phases. No region U was observed with poly (dG).poly (dC). In polynucleotides with alternating nucleotide sequence, the rate of opening of the double helix is strongly dependent on the electrode potential in region U, while in homopolymer pairs, this rate is less potential-dependent. It has been assumed that the difference in the behaviour between homopolymer pairs and polynucleotides with alternating nucleotide sequence is due to differences in absorbability of the two polynucleotide chains in the molecule of a homopolymer pair (resulting from different absorbability of purine and pyrimidine bases) in contrast to equal adsorbability of both chains in a polynucleotide molecule with alternating nucleotide sequence. It has been shown that the mercury electrode is a good model of biological surfaces (e.g. membranes), and that the nucleotide sequence-dependent opening (unwinding) of the DNA double helix at electrically charged surfaces may play an important role in many biological processes.     

The adsorption of DNA in the mercury electrolyte interface. 3. Reaction of DNA in the mercury-electrolyte interface

The adsorption of deoxyribonucleic acid in the mercury-electrolyte interface was investigated. The effect of this adsorption on the differential capacity of the electrical double layer at the interface between a stationary mercury drop electrode (HMDE) and a buffered aqueous sodium chloride solution was measured. The dependences of this differential capacity on potential, time, and pH was studied in the presence of native and also of denatured DNA. These results were compared with the adsorption of model compounds and with the general theory of the adsorption of polymers. The structure of the adsorbed DNA molecules corresponds to an alternating arrangement of two-dimensional, totally adsorbed sequences and three-dimensional loops extending into the solution. The adsorbed sequences and loops consist of several segments with a specific free-energy change of adsorption. Essentially this energy determines the distribution of the segments between adsorbed sequences and loops. The absolute value of this energy change per segment is fairly large in the case of negatively charged poly-electrolyte DNA at the weakly positively charged interface near the electrocapillary maximum (ECM). The fraction of totally adsorbed segments is relatively large in this potential region. The more negative the potential the lower is the absolute value of free energy change of adsorption per segment. Under the conditions unfavorable for the adsorption, only a few segments can be adsorbed. Most of the segments of the adsorbed DNA molecules extend into the solution and therefore fairly high interface concentrations can be reached. Thus, the arrangement of DNA molecules in the electrode surface is changed when the potential is altered from values near the ECM to more negative ones. This change should produce the wave on the differential capacity curves at a little more negative potential than that of ECM. At a more negative potential, intermolecular interactions between the loops extending into the solution may occur. The adsorption tendency of the resulting associates is higher than that of the isolated molecules. Therefore the isolated molecules desorb at sufficient negatively charged interface producing a round wave while the associates stay adsorbed. At this potential it is impossible for native DNA to generate associates because they are formed from the isolated molecules. This explains the hysteresis loop of the curves of differential capacity vs. potential by using the HMDE. The desorption of the associates is indicated by a sharp wave at much more negative potential. For denatured DNA the associates arise from the very few isolated adsorbed molecules at this potential; therefore, no hysteresis loop occurs. The association constant of denatured DNA must be much higher than that of the native DNA. The reasons for this are discussed.     

Some aspects of the copper(II)-DNA interaction

The Cu(II) ion interaction with calf-thymus DNA was studied by means of differential pulse polarography and sweep voltammetry as well as chromatography and viscosimetry. Most of the complexes formed at high ionic strength (0.2 M) and lower Cu(II) concentrations are of a nondenaturing nature. Their formation has but a minor effect on unwinding process of the DNA double helix. The excess of Cu(II) (P = 5) leads, however, to distinct denaturation of the DNA structure. Metal ions have little effect on the denaturation induced by the polarographic reduction of DNA on the mercury electrode. This conclusion is consistent with the character of the polarographic process and with the fact that Cu(II) ions are not very effective in the interaction with AT pairs. Cupric ions have no renaturing ability towards thermally denatured DNA at 0.2 M ionic strength but distinct renaturation was observed at low ionic strength (0.05 M).     

Electrophoresis of adsorbed DNA

The electrophoresis mobilities of native calf thymus DNA adsorbed on the charged solid particles were measured by a micro-electrophoretic method as functions of pII, ionic strength, and DNA concentration. The mobility data confirm the adsorption of DNA both on the positively charged alumina and negatively charged resin particles at wide range of pH and ionic strength. The mobility data also indicate significant DNA adsorption by negatively charged glass in the acidic range of pH. The electrophoretic mobilities of DNA adsorbed on different substrate particles under identical conditions do not differ widely, indicating the major role of the adsorbed DNA rather than the covered substrate in controlling the charge behavior of the particle. The mobilities of the adsorbed DNA at salt pH are of a comparable order of magnitude to those for the dissolved DNA in solution. The mobility of the adsorbed heat-denatured and alkali-denatured DNA is lower than that of the native adsorbed DNA under identical conditions of pH and ionic strength.     

Polarography of Polynucleotides: III. Polyadenylic Acid: The Electrode Process and Interaction with Polyamines

Polyadenylic acid (poly A) was studied under various conditions using both DC polarography and phase sensitive AC polarography and by measuring the time-course of the current during the lifetime of a single drop of the dropping mercury electrode. Under certain conditions the current at potentials of the limiting portion of the DC polarographic wave does not reach its limiting value and in extreme situations peak-shaped curves are observed. This phenomenon is explained in terms of desorption and repulsion from the electrode of neutral poly A due to its polyanionic character. Consequently, the suppression of the current can be enhanced by increasing negative potential of the electrode and by exposing the negative charges of phosphate groups, e.g., by increasing pH and temperature and by decreasing ionic strength and buffer capacity; vice versa, the current suppression can be at least partially eliminated by reversing these conditions. Polyamines which seem to shield the phosphate groups through specific interactions are very effective in eliminating the current suppression. The effectiveness of a polyamine is determined by its chain length and by the density of its amino groups and the geometry of their distribution.     

An electrochemical analysis of changes in properties of DNA caused by ionizing and ultraviolet radiations

Summary Electrooxidation and electroreduction of- and u.v.-irradiated DNA were studied by means of differential pulse voltammetry at the graphite electrode and differential pulse polarography at the dropping mercury electrode. Two separated voltammetric oxidation peaks G and A were used for monitoring conformational changes in guanine - cytosine (GC) and adenine - thymine (AT) pairs respectively in irradiated double-stranded (ds) DNA. Pulse-polarography reduction peak III was used for detection of denatured DNA in the irradiated samples of ds DNA. It was found that the heights of peaks G and A of ds DNA did not change with the radiation dose after relatively low doses of- and u.v.-radiations (up to ca. 40 krads and 1 × 10⁴ Jm^–2, respectively), when no single-stranded (ss) DNA was detected in the irradiated DNA samples. After higher doses of radiation the occurrence of ss DNA or ss segments in the irradiated samples of ds DNA was accompanied by an increase of peaks G and A; however, peak A grew more rapidly with the increasing dose than peak G. It was concluded that the results obtained support the assumption, according to which regions of ds DNA rich in AT pairs are more susceptible to denaturation caused by- and u.v.-radiations.This dose concerns the DNA solution at a concentration of 600 µg/ml^–1     

Adsorption of peptide nucleic acid and DNA decamers at electrically charged surfaces.

Adsorption behavior of peptide nucleic acid (PNA) and DNA decamers (GTAGATCACT and the complementary sequence) on a mercury surface was studied by means of AC impedance measurements at a hanging mercury drop electrode. The nucleic acid was first attached to the electrode by adsorption from a 5-microliter drop of PNA (or DNA) solution, and the electrode with the adsorbed nucleic acid layer was then washed and immersed in the blank background electrolyte where the differential capacity C of the electrode double layer was measured as a function of the applied potential E. It was found that the adsorption behavior of the PNA with an electrically neutral backbone differs greatly from that of the DNA (with a negatively charged backbone), whereas the DNA-PNA hybrid shows intermediate behavior. At higher surface coverage PNA molecules associate at the surface, and the minimum value of C is shifted to negative potentials because of intermolecular interactions of PNA at the surface. Prolonged exposure of PNA to highly negative potentials does not result in PNA desorption, whereas almost all of the DNA is removed from the surface at these potentials. Adsorption of PNA decreases with increasing NaCl concentration in the range from 0 to 50 mM NaCl, in contrast to DNA, the adsorption of which increases under the same conditions.     

Redox protein electron-transfer mechanisms: electrostatic interactions as a determinant of reaction site in c-type cytochromes

The effect of ionic strength on the rate constant for electron transfer has been used to determine the magnitude and charge sign of the net electrostatic potential which exists in close proximity to the sites of electron transfer on various c-type cytochromes. The negatively charged ferricyanide ion preferentially reacts at the positively charged exposed heme edge region on the front side of horse cytochrome c and Paracoccus cytochrome c2. In contrast, at low ionic strength, the positively charged cobalt phenanthroline ion interacts with the negatively charged back side of cytochrome c2, and at high ionic strength at a positively charged site on the front side of the cytochrome. With horse cytochrome c, over the ionic strength range studied, cobalt phenanthroline reacts only at a positively charged site which is probably not at the heme edge. These inorganic oxidants do not react at the relatively uncharged exposed heme edge sites on Azotobacter cytochrome c5 and Pseudomonas cytochrome c-551, but rather at a negatively charged site which is away from the heme edge. The results demonstrate that at least two electron-transferring sites on a single cytochrome can be functional, depending on the redox reactant used and the ionic strength. Electrostatic interactions between charge distributions on the cytochrome surface and the other reactant, or interactions involving uncharged regions on the protein(s), are critical in determining the preferred sites of electron transfer and reaction rate constants. When unfavorable electrostatic effects occur at a site near the redox center, less optimal sites at a greater distance can become kinetically important.     

Plasmid DNA adsorption on silica: kinetics and conformational changes in monovalent and divalent salts

A quartz crystal microbalance with dissipation (QCM-D) is used to determine the adsorption rate of a supercoiled plasmid DNA onto a quartz surface and the structure of the resulting adsorbed DNA layer. To better understand the DNA adsorption mechanisms and the adsorbed layer physicochemical properties, the QCM-D data are complemented by dynamic light scattering measurements of diffusion coefficients of the DNA molecules as a function of solution ionic composition. The data from simultaneous monitoring of variations in frequency and dissipation energy with the QCM-D suggest that the adsorbed DNA layer is more rigid in the presence of divalent (calcium) cations compared to monovalent (sodium) cations. Adsorption rates are significantly higher in the presence of calcium, attaining a transport-limited rate at about 1 mM Ca2+. Results further suggest that in low ionic strength solutions containing 1 mM Ca2+ and in moderately high ionic strength solutions containing 300 mM NaCl, plasmid DNA adsorption to negatively charged mineral surfaces is irreversible.     

Adsorption of bacteriophage on bacterial surface and on the surface of Hg dropping electrode

Summary The influence of the ionic strength of the medium on the adsorption of bacteriophage T 2 to the surfaces of a mercury dropping electrode on one hand and ofbacteria E. coli B on the other hand was studied. The adsorption on the mercury surface was determined by measurement of the differential capacity of the electrode double layer, the adsorption to bacteria was estimated from the decrease of free phage particles in a bacterial suspension with time. The adsorption to the mercury electrode increases with increasing ionic strength of the medium, but adsorption to the surface of bacteria increases at first, has a maximum at concentrations between 0,1 to 0,5 M and decreases with further increase of ionic strength. The decrease of adsorption of phage to the bacterial surface is assumed to be caused by the blocking of specific sites on the bacterial surface by adsorbed ions which sterically prevent the adsorption of the phage. Such specific sites are not present on the electrode surface, therefore adsorption increases further with increasing ionic strength probably due to the neutralization of surface charges of the phage and of the electrode. The saturated surface-concentration of the phage _s was calculated from the dependence of the differential capacity on the concentration. It is concluded from _s value obtained that the phage particles are scattered with wide intervals on the electrode surface with a degree of coverage of approximately 140.Abbreviations used DNA deoxyribonucleic acid - N Avogadro number The authors wishes to express their gratitude to the late Prof.Ferdinand Hercík, director of the Institute of Biophysics, for the initiation of this work and stimulating interest. The authors are also indebted to Dr. J.Koudelka for his kind gift of phage T 2 sample and to Dr. M.Vízdalová for her valuable comments during preparation of this article.     

The interaction of ribonuclease T 1 with DNA.

The interaction of RNase T1 with calf thymus DNA was studied using uv difference spectroscopy and the effect of the enzyme on DNA melting. There was no indication of RNase T1 binding with native DNA. A prominent difference spectrum for RNase T1 binding with denatured DNA (d-DNA) was observed at pH 5, 25 degrees and low ionic strength (mu = .01 M) which was depressed at higher ionic strength and pH. The normalized difference spectrum at mu = .01 M, pH 5 and 25 degrees can be interpreted as indicating an interaction of an exposed guanine residue directly with the enzyme and a coupling of this process with the "melting" of short folded segments of d-DNA. The apparent association constant calculated per M guanine residues was 2.4 X 10-4 M-1 under these conditions. The results are discussed in reference to comparable studies on the interaction of RNase T1 with RNA and small guanine ligands.     

Electrophoresis of absorbed RNA

The electrophoretic mobilities of adsorbed yeast ribonucleic acid have been measured as functions of pH, ionic strength, and biopolymer concentration and the results so obtained have been critically compared with those for adsorbed DNA. Like DNA, ribonucleic acid has also been found to reverse the positive charge of alumina owing to its adsorption on the solid-liquid interface. The mobilities of adsorbed RNA have been found to be less than those of adsorbed DNA under identical conditions. The observed mobilities of adsorbed heat- and alkali-denatured RNA are significantly less than those of adsorbed native RNA at a given pH and ionic strength of the medium. The electrophoretic mobilities as observed also show the evidence of RNA adsorption on the negatively charged surface of Dowex-50 resin, but practically no adsorption of RNA on the negatively charged glass surface has been predicted.     

Studies on electron transfer between mercury electrode and hemoprotein.

The electrochemical behaviour of ferricytochrome c, metmyoglobin and methemoglobin was studied using d.c., a.c. and differential pulse polarography, and controlled potential electrolysis. 1. The three hemoproteins yield d.c. polarographic steps, and peaks in differential pulse polarograms, the height of which is proportional to concentration. The charge transfer is influenced by strong adsorption. 2. The concentration dependence of the a.c. polarograms indicates structural changes in the adsorbed molecules. 3. The reduction products of controlled potential electrolysis of metmyoglobin and methemoglobin have absorption spectra identical with the native control samples. The affinity for oxygen and the cooperativity in hemoglobin are not affected by the reaction at the electrode. 4. The charge transfer proceeds via adsorbed, already reduced, molecules to freely diffusible proteins.     

Adsorption behavior of globular proteins at the water/mercury interface.

The adsorption of globular proteins at solid/liquid or liquid/liquid interfaces provides evidence of unfolded molecular conformation. Proteins with high apolar character are strongly unfolded, while those with high polar character are generally incompletely unfolded. Structural changes of globular proteins at adsorption on mercury electrodes were studied by ac polarography and capacity–time curves. The surface area per molecule of nine globular proteins was determined from the adsorption kinetics at the dropping mercury electrode. For all the proteins investigated, this value was greater than the maximal molecular cross section of the native proteins. The surface area was about 19 Ų per amino acid residue, which coincides with the value for unfolded proteins at the water/air interface. Differences between dropping mercury electrode and hanging drop mercury electrode occurred only with lysozyme and phosphorylase; for the other proteins, the structure of the adsorption layer was independent of the time of interaction at the electrode. Since not all of the reducible groups of the adsorbed proteins come into contact with the electrode, the flattening should be incomplete.     

The effects of surface charges on the redox potential of cytochrome c2 from the purple phototrophic bacterium Rhodobacter capsulatus.

Four site-directed mutants of Rhodobacter capsulatus cytochrome c2, which substitute lysines at three positions with aspartate or glutamate, have been prepared. Mutations included the single charge substitutions K12D, K14E, and K32E and a double charge substitution K14E/K32E. Characterization of the ionic strength dependence of the wild-type and mutant redox potentials in the "nonbinding" buffer Tris-cacodylate suggests that (i) at zero ionic strength introduction of negatively charged groups stabilizes the oxidized state by 11-14 mV per charge and (ii) at high ionic strengths where the charged groups are masked, the effects of single charge substitutions are overcome; however, the redox potential of the double charge substitution is still affected. These results indicate that at physiological ionic strengths charge distribution only affects redox potential when the heme environment has been perturbed by a structural perturbation and that the determinants of redox potential in c-type cytochromes is primarily due to the local heme environment.     

Comparison of the physical properties and assembly pathways of the related bacteriophages T7, T3 and phi II

To understand constraints on the evolution of bacteriophage assembly, the structures, electrophoretic mobilities (mu) and assembly pathways of the related double-stranded DNA bacteriophages T7, T3 and phi II, have been compared. The characteristics of the following T7, T3 and phi II capsids in these assembly pathways have also been compared: (1) a DNA-free procapsid (capsid I) that packages DNA during assembly; (b) a DNA packaging-associated conversion product of capsid I (capsid II). The molecular weights of the T3 and phi II genomes were 25.2 X 10(6) and 25.9 (+/- 0.2) X 10(6) (26.44 X 10(6) for T7, as previously determined), as determined by agarose gel electrophoresis of intact genomes. The radii of T7, T3 and phi II bacteriophages were indistinguishable by sieving during agarose gel electrophoresis (+/- 4%) and measurement of the bacteriophage hydration (+/- 2%) (30.1 nm for T7, as previously determined). Assuming a T = 7 icosahedral lattice for the arrangement of the major capsid subunits (p10A) of T7, T3 and phi II best explains these data and data previously obtained for T7. At pH 7.4 and an ionic strength of 1.2, the solid-support-free mu values (mu 0 values) of T7, T3 and phi II bacteriophages, obtained by extrapolation of mu during agarose gel electrophoresis to an agarose concentration of 0 and correction for electro-osmosis, were -0.71, -0.91 and -1.17(X 10(-4) cm2V-1 s-1. The mu 0 values of T7, T3 and phi II capsids I were -1.51, -1.58 and -2.07(X 10(-4] cm2V-1 s-1. For the capsids II, these mu 0 values were -0.82, -1.07 and -1.37(X 10(-4] cm2V-1 s-1. The tails of all three bacteriophages were positively charged and the capsid envelopes (heads) were negatively charged. In all cases the procapsid had a negative mu 0 value larger in magnitude than the negative mu 0 value for bacteriophage or capsid II. A trypsin-sensitive region in capsid I-associated, but not capsid II-associated, T3 p10A was observed (previously observed for T7). The largest fragment of trypsinized capsid I-associated p10A had the same molecular weight in T7 and T3, although the T3 p10A is 18% more massive than the T7 p10A. It is suggested that the trypsin-resistant region of capsid I-associated p10A determines the radius of the bacteriophage capsid.