The sieving of spheres during agarose gel electrophoresis: quantitation and modeling

By use of agarose gel electrophoresis, the sieving of spherical particles in agarose gels has been quantitated and modeled for spheres with a radius (R) between 13.3 and 149 nm. For quantitation, the electrophoretic mobility has been determined as a function of agarose percentage (A). Because a previously used model of sieving [D. Rodbard and A. Chrambach (1970) Proc. Natl. Acad. Sci. USA 65, 970-977] was found incompatible with some of these data, alternative models have been tested. By use of an underivatized agarose, two models, both based on the assumption of a single effective pore radius (PE) for each A, were found to yield PE values that were independent of R and that were in agreement with values of PE obtained independently (PE = 118 nm X A-0.74): sieving by altered hydrodynamics in a cylindrical tube of radius, PE, and sieving by steric exclusion from a circular hole of radius, PE. The same analysis applied to a 6.5% hydroxyethylated commercial agarose yielded a steeper PE vs A plot and also agreement of the above two models with the data. The PE vs A plot was significantly altered by both further hydroxyethylation and factors that cause variation in the electro-osmosis found in commercial agarose.     

The sieving of rod-shaped viruses during agarose gel electrophoresis. I. Comparison with the sieving of spheres

The sieving of rod-shaped viruses during agarose gel electrophoresis is quantitatively analyzed here with a previously proposed model [G. A. Griess et al. (1989) Biopolymers, 28, 1475-1484] that has one radius (PE) of the effective pore at each concentration of gel. By use of this model and an internal spherical size standard, a plot of electrophoretic mobility vs agarose percentage is converted to a plot of the radius of the effective sphere (effective radius) vs PE. Experimentally, when the concentration of the rod-shaped bacteriophage, fd, is progressively increased, eventually the electrophoretic mobility of fd becomes dependent on its concentration. The concentration of fd at which this occurs decreases as the agarose concentration decreases. After avoiding this dependence on the concentration of sample, the effective radius of rod-shaped particles, including bacteriophage fd, length variants of fd, and length variants of tobacco mosaic virus, is found to increase as PE increases until a plateau of approximately constant maximum effective radius is reached at PcE. In the region of this plateau, the effective sphere's measure that best approximates that of the rod is surface area. However, significant disagreement with the data exists for surface area; the maximum effective radius for fd varies as (length)0.69. For fd and its length variants, the value of 2.PcE/length increases from 0.21 to 0.86 as the length decreases from 2808 to 367 nm. The dependence of effective radius on PE and the proximity of 2.PcE to the length of the rod are explained by (a) random orientation of rods at PE values in the region of the plateau, and (b) increasingly preferential end-first orientation (reptation) of the rod as PE decreases below PcE. This hypothesis of reptation is supported by a significant dependence of electrophoretic mobility on electrical potential gradient for a PE below, but not above, PcE. The dependence of 2.PcE/length on length is not rigorously understood, but is qualitatively explained by flexibility of the rods. This apparent flexibility has thus far prevented determination of a rod's axial ratio from quantitation of sieving during agarose gel electrophoresis. The electrical potential dependence of electrophoretic mobility is determined here by a procedure of two-dimensional agarose gel electrophoresis. This procedure is also useful for detecting rod-shaped particles in heterogeneous mixtures of predominantly spherical particles.     

Detection and characterization of agarose-binding, capsid-like particles produced during assembly of a bacteriophage T7 procapsid.

It has previously been shown that: (i) during infection of its host, the DNA bacteriophage T7 assembles a DNA-free procapsid (capsid I), a capsid with an envelope differing physically and chemically from the capsid of the mature bacteriophage, and (ii) capsid I converts to a capsid (capsid II) with a bacteriophage-like envelope as it packages DNA. Lysates of phage T7-infected Escherichia coli contained a particle (AG particle) which copurified with capsid II during buoyant density sedimentation, velocity sedimentation, and solid support-free electrophoresis, but was distinguished from capsid II by its apparent diversity during electrophoresis in agarose gels. Treatment of AG particles with trypsin converted most of them to particles that comigrated with trypsin-treated capsid II during electrophoresis in agarose gels. Irreversible binding of AG particles to agarose gels was shown to contribute to the apparent diversity of AG particles during agarose gel electrophoresis. The results of quantitation of AG particles and of capsid I and capsid II in lysates of a nonpermissive host infected with T7 amber mutants suggested that, in site of their capsid II-like properties, most AG particles were produced during assembly of capsid I and not during DNA packaging. The presence of AG particles in T7 lysates explains contradictions in previous data concerning the pathway of T7 assembly.     

Gel electrophoresis of micron-sized particles: a problem and a solution

The gel electrophoresis of spherical particles with a radius above 0.2 micron has not been reported yet. In the present study, video phase-contrast light microscopy is used to observe the motion of individual latex spheres, 0.52 micron in radius, during electrophoresis in 0.1% agarose gels. At 2 V/cm, the spheres initially migrate in the direction of the electrical field. However, each sphere eventually undergoes a cessation of all motion. Brownian motion is restored when the electrical potential gradient is reduced to zero. Arrest can be prevented by periodically inverting the direction of the electrical field. These observations are explained by electrical field-induced steric trapping of the spheres by gel fibers. Inversion of the electrical field should assist the application of agarose gel electrophoresis to micron-sized cellular organelles and cells.     

Improvements in procedures for electrophoresis in dilute agarose gels

Procedures have been developed for performing electrophoresis in agarose gels with agarose concentrations as low as 0.035%. Using these procedures, agarose gel electrophoresis of the following has been performed: (a) bacteriophage T7 missing its tail fibers; no detectable sieving of this spherical particle (radius = 30.1 nm) occurred below 0.075% agarose, (b) duplex DNAs with molecular weights between 26.5 × 10⁶ and 110 × 10⁶.     

Exclusion of spheres by agarose gels during agarose gel electrophoresis: dependence on the sphere's radius and the gel's concentration

Agarose gel electrophoresis of spheres (radius = R) has been used to determine the effective radius (PE) of the pores of an agarose gel (percentage of agarose in a gel = A). The value of PE at a given A was taken to be the R of the largest sphere that enters the gel. When log PE is plotted as a function of log A, the results can be represented by: PE = 118A-0.74 for 0.2 less than or equal to A less than or equal to 4.0 (PE in nm). However, the data suggest significant nonlinearity in this plot, the magnitude of the exponent of the PE vs A relationship increasing by about 20% as A increases from 0.2 to 4.0. From these data, PE's as big as 1500 nm and as small as 36 nm can be achieved with agarose gels formed with unmodified, unadulterated agarose and usable for electrophoresis.     

Function of an internal bacteriophage T7 core during assembly of a T7 procapsid.

A DNA-free, proteinaceous procapsid of bacteriophage T7 (capsid I) has been shown in previous studies to consist of an external, spherical shell (envelope) and an internal, cylindrical core with fibrous projections that connect the core to the envelope. To determine the role of the core in assembly of the envelope of capsid I, the kinetics of appearance of capsid I and possible intermediates in capsid I assembly (AG particles) were determined in the presence and absence of the core. For obtaining these data, agarose gel electrophoresis was used and appeared to be a technique more accurate and efficient than techniques used for obtaining similar data in the past. The results of these experiments were: (i) in the presence of the core, AG particles behaved kinetically as intermediates in the assembly of capsid I; (ii) in the absence of the core, assembly of capsid I terminated prematurely and AG particles accumulated. These and other data have been interpreted by assuming that: AG particles are breakdown products of precursors of capsid I; these precursors have uncorrected errors in the assembly of their envelope; and a function of the core is to correct these errors.     

Stability and morphology comparisons of self-assembled virus-like particles from wild-type and mutant human hepatitis B virus capsid proteins

Instead of displaying the wild-type selective export of virions containing mature genomes, human hepatitis B virus (HBV) mutant I97L, changing from an isoleucine to a leucine at amino acid 97 of HBV core antigen (HBcAg), lost the high stringency of selectivity in genome maturity during virion export. To understand the structural basis of this so-called "immature secretion" phenomenon, we compared the stability and morphology of self-assembled capsid particles from the wild-type and mutant I97L HBV, in either full-length (HBcAg1-183) or truncated core protein contexts (HBcAg1-149 and HBcAg1-140). Using negative staining and electron microscopy, full-length particles appear as "thick-walled" spherical particles with little interior space, whereas truncated particles appear as "thin-walled" spherical particles with a much larger inner space. We found no significant differences in capsid stability between wild-type and mutant I97L particles under denaturing pH and temperature in either full-length or truncated core protein contexts. In general, HBV capsid particles (HBcAg1-183, HBcAg1-149, and HBcAg1-140) are very robust but will dissociate at pH 2 or 14, at temperatures higher than 75 degrees C, or in 0.1% sodium dodecyl sulfate (SDS). An unexpected upshift banding pattern of the SDS-treated full-length particles during agarose gel electrophoresis is most likely caused by disulfide bonding of the last cysteine of HBcAg. HBV capsids are known to exist in natural infection as dimorphic T=3 or T=4 icosahedral particles. No difference in the ratio between T=3 (78%) and T=4 particles (20.3%) are found between wild-type HBV and mutant I97L in the context of HBcAg1-140. In addition, we found no difference in capsid stability between T=3 and T=4 particles successfully separated by using a novel agarose gel electrophoresis procedure.     

A small (58-nm) attached sphere perturbs the sieving of 40-80-kilobase DNA in 0.2-2.5% agarose gels: analysis of bacteriophage T7 capsid-DNA complexes by use of pulsed field electrophoresis.

Although the icosahedral bacteriophage T7 capsid has a diameter (58 nm) that is 234-fold smaller than the length of the linear, double-stranded T7 DNA, binding of a T7 capsid to T7 DNA is found here to have dramatic effects on the migration of the DNA during both pulsed field agarose gel electrophoresis (PFGE; the field inversion mode is used) and constant field agarose gel electrophoresis (CFGE). For these studies, capsid-DNA complexes were obtained by expelling DNA from mature bacteriophage T7; this procedure yields DNA with capsids bound at a variable position on the DNA. When subjected to CFGE at 2-6 V/cm in 0.20-2.5% agarose gels, capsid-DNA complexes arrest at the electrophoretic origin. Progressively lowering the electrical potential gradient to 0.5 V/cm results in migration; most complexes form a single band. The elevated electrical potential gradient (3 V/cm) induced arrest of capsid-DNA complexes is reversed when PFGE is used instead of CFGE. For some conditions of PFGE, the mobility of capsid-DNA complexes is a function of the position of the capsid on the DNA. During either CFGE (0.5 V/cm) or PFGE, capsid-DNA complexes increasingly separate from capsid-free DNA as the percentage of agarose increases. During these studies, capsid-DNA complexes are identified by electron microscopy of enzymatically-digested pieces of agarose gel; this is apparently the first successful electron microscopy of DNA from an agarose gel.(ABSTRACT TRUNCATED AT 250 WORDS)     

High density lipoprotein particle size distribution in subjects with obstructive jaundice

High density lipoproteins (HDL) from 14 patients with obstructive jaundice were examined by gradient gel electrophoresis to determine the effect of obstruction on particle size distribution. HDL from 7 of these patients were fractionated by gel permeation chromatography and further characterized by electron microscopy, SDS gel electrophoresis, apolipoprotein A-I and apolipoprotein A-II immunoturbidimetry, and analysis of chemical composition. In addition, lecithin:cholesterol acyltransferase (LCAT) activity was measured and correlated with plasma apolipoprotein A-I concentration and particle size distribution. HDL were abnormal in all patients regardless of severity, cause, or duration of obstruction. The major HDL subfraction in normal subjects, HDL3a (radius 4.1-4.3 nm) was either absent or considerably diminished, and HDL2b (radius 5.3 nm) was also frequently absent. Very small particles comparable in size to normal HDL3c (radius 3.8 nm) were prominent. In patients with a bilirubin concentration greater than 250 mumol/l, normal HDL had totally disappeared and were replaced by large discoidal particles of radius 8.5 nm and small spherical particles of radius 3.6-3.7 nm. Both populations of particles were markedly depleted of cholesteryl ester and enriched in free cholesterol and phospholipid. The discoidal particles were rich in apolipoproteins E, A-I, A-II, and C, while the small spherical particles contained predominantly apolipoprotein A-I. LCAT activity was diminished in all subjects to 8-54% of normal, and was strongly positively correlated (r = 0.91 P less than 0.05) with plasma apolipoprotein A-I levels.     

Isolation and characterization of a new dsRNA virus fromWickerhamia fluorescens

Virus-like particles (VLPs) were isolated from the yeastWickerhamia fluorescens strain CCY61-1-1. The VLPs are approximately 42 nm in diameter and contain only one species of dsRNA molecule. The apparent length of the dsRNA determined by native agarose gel electrophoresis was 4.6 kbp. Analysis of protein content of the VLPs showed them to contain one major capsid protein with an apparent molar mass of 74.5 kDa.     

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.     

Size determination of multienzyme complexes using two-dimensional agarose gel electrophoresis

In studies of the size and structure of multienzyme complexes, a procedure complementary to electron microscopy for determining the molecular dimensions of hydrated multisubunit complexes is needed. For some applications this procedure must be capable of detecting aggregation of complexes and must be applicable to impure preparations. In the present study, a procedure of two-dimensional agarose gel electrophoresis (2d-AGE) (Serwer, P. et al. Anal. Biochem. 152:339-345, 1986) was modified and employed to provide accurate size measurements of several classical multienzyme complexes. To improve band clarity and to achieve required gel pore sizes, a hydroxyethylated agarose was used. The effective pore's radius (PE) as a function of gel concentration was determined for this agarose in the range of PE values needed for multienzyme complexes (effective radius, R = 10-30 nm). Appropriate conditions were established to measure R values +/- 1% of the pyruvate (PDC), alpha-ketoglutarate (alpha-KGDC), and the branched chain alpha-keto acid (BCDC) dehydrogenase multienzyme complexes; the accuracy of R was limited by the accuracy of the determinations of the R value for the size standards. The PDC from bovine heart was found to have an R = 22.4 +/- 0.2 nm following cross-linking with glutaraldehyde that was necessary for stabilization of the complex. Dimers and trimers of PDC, present in the preparations used, were separated from monomeric PDC during 2d-AGE.(ABSTRACT TRUNCATED AT 250 WORDS)     

Bacteriophage P22 capsids with a subgenome length of packaged DNA

Bacteriophage P22 assembles a DNA-free procapsid that subsequently packages P22 DNA. To study the packaging of bacteriophage P22 DNA, attempts were made to isolate P22 capsids with a subgenome length of packaged DNA. With the use of cesium chloride buoyant density sedimentation and agarose gel electrophoresis, the following capsids with a subgenome length of packaged DNA were isolated and characterized: (i) a capsid with the solid-support-free electrophoretic mobility and radius of the DNA-free P22 procapsid; (ii) a capsid with the solid-support-free electrophoretic mobility and radius of the mature P22 bacteriophage; and (iii) a capsid with a solid-support-free electrophoretic mobility and possibly a radius intermediate to those of the procapsid and bacteriophage.     

A technique for electrophoresis in multiple-concentration agarose gels

A technique has been developed for embedding several agarose gels (running gels), each of a different agarose concentration, within a single 1.5% agarose slab. Equal portions of a sample were placed at the origin of each running gel and were simultaneously subjected to electrophoresis. Protein within the running gels was detected by staining with Coomassie blue; 0.2% gels were the least concentrated gels that were stained without gel breakage. Using the above technique, the dependence of electrophoretic mobility on agarose concentration has been measured for bacteriophage T7 capsids and a capsid dimer.     

Size effects on diffusion processes within agarose gels

To investigate diffusion processes in agarose gel, nanoparticles with sizes in the range between 1 and 140 nm have been tested by means of fluorescence correlation spectroscopy. Understanding the diffusion properties in agarose gels is interesting, because such gels are good models for microbial biofilms and cells cytoplasm. The fluorescence correlation spectroscopy technique is very useful for such investigations due to its high sensitivity and selectivity, its excellent spatial resolution compared to the pore size of the gel, and its ability to probe a wide range of sizes of diffusing nanoparticles. The largest hydrodynamic radius (R(c)) of trapped particles that displayed local mobility was estimated to be 70 nm for a 1.5% agarose gel. The results showed that diffusion of particles in agarose gel is anomalous, with a diverging fractal dimension of diffusion when the large particles become entrapped in the pores of the gel. The latter situation occurs when the reduced size (R(A)/R(c)) of the diffusing particle, A, is >0.4. Variations of the fractal exponent of diffusion (d(w)) with the reduced particle size were in agreement with three-dimensional Monte Carlo simulations in porous media. Nonetheless, a systematic offset of d(w) was observed in real systems and was attributed to weak nonelastic interactions between the diffusing particles and polymer fibers, which was not considered in the Monte Carlo simulations.     

Electrophoresis of bacteriophage T7 and T7 capsids in agarose gels.

Agarose gel electrophoresis of the following was performed in 0.05 M sodium phosphate-0.001 M MgCl2 (pH 7.4): (i) bacteriophage T7; (ii) a T7 precursor capsid (capsid I), isolated from T7-infected Escherichia coli, which has a thicker and less angular envelope than bacteriophage T7; (iii) a second capsid (capsid II), isolated from T7-infected E. coli, which has a bacteriophage-like envelope; and (iv) capsids (capsid IV) produced by temperature shock of bacteriophage T7. Bacteriophage T7 and all of the above capsids migrated towards the anode. In a 0.9% agarose gel, capsid I had an electrophoretic mobility of 9.1 +/- 0.4 X 10(-5) cm2/V.s; bacteriophage T7 migrated 0.31 +/- 0.02 times as fast as capsid I. The mobilities of different preparations of capsid II varied in such gels: the fastest-migrating capsid II preparation was 0.51 +/- 0.03 times as fast as capsid I and the slowest was 0.37 +/- 0.02 times as fast as capsid I. Capsid IV with and without the phage tail migrated 0.29 +/- 0.02 and 0.42 +/- 0.02 times as fast as capsid I. The results of the extrapolation of bacteriophage and capsid mobilities to 0% agarose concentration indicated that the above differences in mobility are caused by differences in average surface charge density. To increase the accuracy of mobility comparisons and to increase the number of samples that could be simultaneously analyzed, multisample horizontal slab gels were used. Treatment with the ionic detergent sodium dodecyl sulfate converted capsid I to a capsid that migated in the capsid II region during electrophoresis through agarose gels. In the electron microscope, most of the envelopes of these latter capsids resembled the capsid II envelope, but some envelope regions were thicker than the capsid II envelope.     

Assembly of the herpes simplex virus capsid: identification of soluble scaffold-portal complexes and their role in formation of portal-containing capsids

The herpes simplex virus type 1 (HSV-1) portal complex is a ring-shaped structure located at a single vertex in the viral capsid. Composed of 12 U(L)6 protein molecules, the portal functions as a channel through which DNA passes as it enters the capsid. The studies described here were undertaken to clarify how the portal becomes incorporated as the capsid is assembled. We tested the idea that an intact portal may be donated to the growing capsid by way of a complex with the major scaffolding protein, U(L)26.5. Soluble U(L)26.5-portal complexes were found to assemble when purified portals were mixed in vitro with U(L)26.5. The complexes, called scaffold-portal particles, were stable during purification by agarose gel electrophoresis or sucrose density gradient ultracentrifugation. Examination of the scaffold-portal particles by electron microscopy showed that they resemble the 50- to 60-nm-diameter "scaffold particles" formed from purified U(L)26.5. They differed, however, in that intact portals were observed on the surface. Analysis of the protein composition by sodium dodecyl sulfate-polyacrylamide gel electrophoresis demonstrated that portals and U(L)26.5 combine in various proportions, with the highest observed U(L)6 content corresponding to two or three portals per scaffold particle. Association between the portal and U(L)26.5 was antagonized by WAY-150138, a small-molecule inhibitor of HSV-1 replication. Soluble scaffold-portal particles were found to function in an in vitro capsid assembly system that also contained the major capsid (VP5) and triplex (VP19C and VP23) proteins. Capsids that formed in this system had the structure and protein composition expected of mature HSV-1 capsids, including U(L)6, at a level corresponding to approximately 1 portal complex per capsid. The results support the view that U(L)6 becomes incorporated into nascent HSV-1 capsids by way of a complex with U(L)26.5 and suggest further that U(L)6 may be introduced into the growing capsid as an intact portal.     

侵染半夏的两种病毒的分离纯化和初步鉴定

用自然感染的半夏（Ｐｉｎｅｌｌｉａｔｅｒｎａｔａ）为材料,经粗提纯后检查到一种线状病毒和一种球状病毒,用两种方法对担提纯样品中的病毒粒子进行了分离纯化。１０％－７０％连续甘油梯度８００００ｇ离心１５０分钟获得两条病毒带,经紫外吸收测定均为强的核蛋白吸收峰,病毒粒子检查分别为球状和线状病毒粒子,线状病毒经浓缩收集为均一成份．与芋花叶病毒（Ｄａｓｈｅｅｍｍｏｓａｉｃｖｉｒｕｓ,ＤＭＶ）抗体有强的阳性反应。粗提纯样品经０．８％琼脂糖凝胶电脉分离为一条蛋白带,该条带回收后经紫外吸收测定为核蛋白吸收峰,电镜下检查为均一的球状病毒,以ＴＭＶ为对照、醋酸铀（ＵＡＣ）负染后测得该球状病毒（ｐｉｎｅｌｌｉａｓｐｈｅｒｉｃａｌｖｉｒｕｓ１．ＰｓＶ－１）的大小为３１．７ｎｍ;戊二醛固定后磷钨酸（ＰＴＡ）负染测得ＰｓＶ—１的大小为３４．０ｎｍ。各组分经ＳＤＳ－聚丙烯酸胺凝焦电泳分析测得线状病毒和球状病毒的外壳蛋白分子量分别为２０ＫＤ和２８ＫＤ。初步确定线状病毒为ＤＭＶ．球状病毒ＰｓＶ—１为侵梁天南星科半夏的一种新病毒。     

Diffusion of macromolecules in agarose gels: comparison of linear and globular configurations.

The diffusion coefficients (D) of different types of macromolecules (proteins, dextrans, polymer beads, and DNA) were measured by fluorescence recovery after photobleaching (FRAP) both in solution and in 2% agarose gels to compare transport properties of these macromolecules. Diffusion measurements were conducted with concentrations low enough to avoid macromolecular interactions. For gel measurements, diffusion data were fitted according to different theories: polymer chains and spherical macromolecules were analyzed separately. As chain length increases, diffusion coefficients of DNA show a clear shift from a Rouse-like behavior (DG congruent with N0-0.5) to a reptational behavior (DG congruent with N0-2.0). The pore size, a, of a 2% agarose gel cast in a 0.1 M PBS solution was estimated. Diffusion coefficients of the proteins and the polymer beads were analyzed with the Ogston model and the effective medium model permitting the estimation of an agarose gel fiber radius and hydraulic permeability of the gels. Not only did flexible macromolecules exhibit greater mobility in the gel than did comparable-size rigid spherical particles, they also proved to be a more useful probe of available space between fibers.