Ion permeability of rabbit intestinal brush border membrane vesicles

Summary The ion permeability of rabbit jejunal brush border membrane vesicles was studied by measuring unidirectional fluxes with radioactive tracers and bi-ionic diffusion potentials with the potential-sensitive fluorescent dye, diS–C₃-(5). Tracer measurements provide estimates of the absolute magnitudes of permeability coefficients, while fluorescence measurements provide estimates of relative and absolute ion permeabilities. The magnitudes of the permeability coefficients for Na⁺, K⁺, Rb⁺, and Br^– were approximately 5 nanoliters/(mg protein × sec) or 10^–5 cm/sec as determined by radioactive tracer measurements. The apparent selectivity sequence, relative to Na⁺, as determined by bi-ionic potential measurements was: F^–, isetheionate, gluconate, choline (<0.1)+(1.0)–(1.5)=NO ₃ ^– (1.5)–(2.3)+(2.4)+(2.5)+(2.6)+(3.9) 4 ^– +(12)–(40). The origin of this selectivity sequence and its relationship to the ion permeability of the brush border membrane in the intact epithelium are discussed.     

Osmotic water permeabilities of human placental microvillous and basal membranes

Summary Literature data suggest that water accumulation by the human fetus is driven by osmotic gradients of small solutes. However, the existence of such gradients has not been supported by prior measurements. Attempts to estimate the size of the gradient necessary to drive net water movement have been seriously hampered by the lack of permeability data for the syncytiotrophoblast membranes. Stopped-flow light scattering techniques were employed to measure the osmotic water permeability (P _f )of microvillous (MVM) and basal membrane (BM) vesicles isolated from human term placenta. At 37°C, the P _f was determined to be 1.9±0.06 × 10^+–3 cm/sec for MVM and 3.1±0.20 × 10^+–3 cm/sec for BM (mean ±SD, n = 6). At 23°C, P _f was reduced to 0.7±0.04 × 10^+–3 cm/sec in MVM and 1.6±0.05 × 10^+–3 cm/sec in BM. These P _f values are comparable to those observed in membranes where water has been shown to permeate via a lipid diffusive mechanism. Arrhenius plots of P _f over the range 20–40°C were linear, with activation energies of 13.6 ± 0.6 kcal/mol for MVM and 12.9±1.0 kcal/mol for BM. Water permeation was not affected by mercurial sulfhydryl agents and glucose transport inhibitors. These data clearly suggest that water movement across human syncytiotrophoblast membranes occurs by a lipid diffusion pathway. As noted in several other epithelial tissues, the basal membrane has a higher water permeability than the microvillous membrane. It is speculated that water accumulation by the human fetus could be driven by a solute gradient small enough to be within the error of osmolarity measurements.We thank the staff of the labor and delivery ward at University of San Francisco Medical Center for help in obtaining placental tissue. This work was supported by NIH grant HD 26392. Dr. Jansson was supported by the Sweden-America Foundation, The Swedish Society of Medicine, The Swedish Society for Medical Research, and the Swedish Medical Research Council.     

Phosphate permeability in cells ofChlorella ellipsoidea

Summary Active transport of orthophosphate byChlorella ellipsoidea was observed at 25 °C under fluorescent light, about 3 klux. Influx and efflux of phosphate, and extra- and intracellular phosphate concentrations were measured in order to assess phosphate permeability in the cells. The permeability ranged from 10^–3 to 10^–4 mlQ/mg cell min (or 10^–7 to 10^–8cm/sec).     

Evidence for permanent water channels in the basolateral membrane of an ADH-sensitive epithelium

Summary The transepithelial water permeability in frog urinary bladder is believed to be essentially dependent on the ADH-regulated apical water permeability. To get a better understanding of the transmural water movement, the diffusional water permeability (P _d) of the basolateral membrane of urinary bladder was studied. Access to this post-luminal barrier was made possible by perforating the apical membrane with amphotericin B. The addition of this antibiotic increasedP _d from 1.12±0.10×10^–4 cm/sec (n=7) to 4.08±0.33×10^–4 cm/sec (n=7). The effect of mercuric sulfhydryl reagents, which are commonly used to characterize water channels, was tested on amphotericin B-treated bladders. HgCl₂ (10^–3 m) decreasedP _d by 52% andpara-chloromercuribenzoic acid (pCMB) (1.4×10^–4 m) by 34%. The activation energy for the diffusional water transport was found to increase from 4.52±0.23 kcal/mol (n=3), in the control situation, to 9.99±0.91 kcal/mol (n=4) in the presence of 1.4×10^–4 m pCMB. Our second approach was to measure the kinetics of water efflux, by stop-flow light scattering, on isolated epithelial cells from urinary bladders.pCMB (0.5 or 1.4×10^–4 m) was found to inhibit water exit by 91±2%. These data strongly support the existence of proteins responsible for water transport across the basolateral membrane, which are permanently present.     

The basal permeability to water of human red blood cells evaluated by a nuclear magnetic resonance technique

The characteristics of water diffusional permeability (P) of human red blood cells were studied on isolated erythrocytes by a doping nuclear magnetic resonance technique. In order to estimate the basal permeability the maximal inhibition of water diffusion was induced by exposure of red blood cells to p-chloromercuribenzene sulfonate (PCMBS) under various conditions (concentration, duration, temperature). The lowest values of P were around 0.7×10^–3 cm s^–1 at 10°C, 1.2×10^–3 cm s^–1 at 15°C, 1.4×10^–3 cm s^–1 at 20°C, 1.8×10^–3 cm s^–1 at 25°C, 2.1×10^–3 cm s^–1 at 30°C and 3.5×10^–3 cm s^–1 at 37°C. The mean value of the activation energy of water diffusion (E_a,d) was 25 kJ/mol for control and 43.7 kJ/mol for PCMBS-inhibited erythrocytes. The values of P and E_a,d obtained after induction of maximal inhibition of water diffusion by PCMBS can be taken as references for the basal permeability to water of the human red blood cell membrane.     

Permeation characteristics of isolated cuticles of Citrus aurantium L. for monoterpenes

Summary Permeation parameters of isolated cuticular membranes of Citrus aurantium L. for gaseous monoterpenes were determined by an isostatic system. For -pinene and d-limonene permeability coefficients range from 4.3 × 10^–11 m^–2 s^–1 to 7.3 × 10^–11 m^–2 s^–1. These values can be compared to that measured for benzene gas at the cuticle of Citrus. The permeability coefficients of the two monoterpenes did not differ significantly, in contrast to their diffusioin coefficients. The diffusion coefficient values are 3.7 × 10^–15 m^–2 s^–1 for limonene and 15.5 × 10^–15 m^–2 s^–1 for -pinene. The reason for this difference is still unclear. A dependence of the permeation parameters on the direction of the monoterpene transport could not be observed. Moreover, there are some indications that, in spite of its heterogeneous character, the cuticular membrane of Citrus is homogeneous in respect to the transport of small gaseous molecules. An exposure to environmentally relevant ozone concentrations for 6 months did not change the permeation characteristics of the membrane. Due to the high variability of the samples only a tendency towards higher permeability coefficients of cuticles treated with 80 ppb ozone was observed. This may be attributed to a reduced tension of the membrane caused by chain fractions.This paper is dedicated to Prof. Dr. Otto Härtl, Graz, on the occasion of his 80th birthday.     

Permeance of novikoff hepatoma gap junctions: Quantitative video analysis of dye transfer

Summary Fluorescent dyes are commonly used to study permeable (gap) junctions, but only rarely have quantitative values for junctional dye permeability been determined. In the present study, junctional permeance (PA, i.e., the product of the junctional permeability coefficient,P, times the junctional area,A) to Lucifer Yellow CH (LY) has been obtained for pairs of Novikoff hepatoma cells. Dye was microinjected into one cell and the subsequent transfer monitored by a SIT camera and recorded on video tape. The intensities of fluorescence in the injected and recipient cell were measured using a Digisector (Microworks) digitizing board and an Apple II Plus computer to analyze the video records. These changes in intensity, along with an estimate of volume of the spherical cells, were used to calculate the junctional permeance (PA) of cell pairs according to Fick's diffusion equation. Junctional permeances show considerable variation ranging from 0.08×10^–11 to 27.0×10^–11 cm³/sec. Using the meanPA and a previous estimate of the mean number of junctional channels per interface in the Novikoff cultures, a value for diffusion coefficient of LY through gap junctions is calculated to be about 1.4×10^–6 cm²/sec. There is a general proportionality between meanPA and cell volume for hepatoma cell pairs of a certain size range. Such a relationship between cell volume and junctional capacity suggests one source of variation ofPA. Other possible sources, e.g., related to position in the cell cycle, are discussed.     

Frog striated muscle is permeable to hydroxide and buffer anions

Hydroxide, bicarbonate and buffer anion permeabilities in semitendinosus muscle fibers of Rana pipiens were measured. In all experiments, the fibers were initially equilibrated in isotonic, high K₂SO₄ solutions at pH _o =7.2 buffered with phosphate. Two different methods were used to estimate permeabilities: (i) membrane potential changes were recorded in response to changes in external ion concentrations, and (ii) intracellular pH changes were recorded in response to changes in external concentrations of ions that alter intracellular pH. Constant field equations were used to calculate relative or absolute permeabilities.In the first method, to increase the size of the membrane potential change produced by a sudden change in anion entry, external K⁺ was replaced by Cs⁺ prior to changes of the anion under study. At constant external Cs⁺ activity, a hyperpolarization results from increasing external pH from 7.2 to 10.0 or higher, using either CAPS (3-[cyclohexylamino]-1-propanesulfonic acid) or CHES (2-[N-cyclohexylamino]-ethanesulfonic acid) as buffer. For each buffer, the protonated form is a zwitterion of zero net charge and the nonprotonated form is an anion. Using reported values of H⁺ permeability, calculations show that the reduction in [H⁺] _o cannot account for the hyperpolarizations produced by alkaline solutions. Membrane hyperpolarization increases with increasing total external buffer concentration at constant external pH, and with increasing external pH at constant external buffer anion concentration. Taken together, these observations indicate that both OH^– and buffer anions permeate the surface membrane. The following relative permeabilities were obtained at pH_o, 10.0± 0.3: (P_OH/P_K) = 890 ± 150, (P_CAPS/P_K) = 12 ± 2 (P_CHIES/P_K) = 5.3 ± 0.9, and (P_NO3/P_K) = 4.7 ± 0.5 P_NO/P_K was independent of pH _o up to 10.75. At pH_o = 9.6, (P_HCO3/P_K) = 0.49 ± 0.03; at pH _o = 8.9, (P_Cl/P_K) = 18± 2 and at pH _o = 7.1, (P_HEPES/P_K) = 20 ± 2.In the second method, on increasing external pH from 7.2 to 10.0, using 2.5 mm CAPS (total buffer concentration), the internal pH increases linearly with time over the next 10 min. This alkalinization is due to the entry of OH^– and the absorption of internal H⁺ by entering CAPS^– anion. The rate of CAPS^– entry was determined in experiments in which the external CAPS concentration was increased at constant external pH. Such increases invariably produced an increase in the rate of internal alkalinization, which was reversed when the CAPS concentration was reduced to its initial value. From the internal buffer power, the diameter of the fiber under study and the rates of change of internal pH, the absolute permeability for both OH^– and CAPS^– were calculated. At external pH = 10.0, the average (±sem) permeabilities were: P_OH=1.68±0.19×10^–4 cm/sec and P_CAPS=2.10±0.74×10^–6cm/sec.We conclude that OH^– is about 50 times more permeable than Cl^– at alkaline pH and that the anionic forms of commonly used buffers have significant permeabilities.This research was supported by a grant from the National Institutes of Health (AR 31814). The authors wish to thank Dr. Peter G. Shrager and Dr. Bruce C. Spalding for reading an early draft of this report and for providing helpful suggestions.     

Ion and sugar permeabilities of lecithin bilayers: Comparison of curved and planar bilayers

Summary Na⁺ and sugar permeabilities of egg lecithin bilayers were measured using curved bilayers and planar bilayers as represented by single-bilayer vesicles and black lipid films, respectively. The Na⁺ permeability coefficient measured with single-bilayer vesicles at 25°C is (2.1±0.6)×10^–13 cm sec^–1. Because of technical difficulties it has been impossible to measure ionic permeabilities of values lower than about 10^–10 cm sec^–1 in planar (black) lipid bilayers using tracer methods. Thed-glucose andd-fructose permeabilities were measured with both curved and planar bilayers. The permeability coefficients measured with vesicles at 25°C are (0.3±0.2)×10^–10 cm sec^–1 for glucose and (4±1)×10^–10 cm sec^–1 ford-fructose; these are in reasonable agreement with the corresponding values obtained for planar (black) lipid bilayers which are (1.1±0.3)×10^–10 cm sec^–1 ford-glucose and (9.3±0.3)×10^–10 cm sec^–1 ford-fructose, respectively.This paper is dedicated to the memory of Walther Wilbrandt,cuius nomini nullum par elogium.     

Nitrate and chloride ions have different permeation pathways in skeletal muscle fibers ofRana pipiens

Summary The effects of pH on the permeability and conductance of the membranes to nitrate and to chloride of semitendinosus and lumbricalis muscle fibers were examined.Membrane potential responses to quick solution changes were recorded in semitendinosus fibers initially equilibrated in isotonic, high K₂SO₄ solutions. External solutions were first changed to ones in which either Rb⁺ or Cs⁺ replaced K⁺ and then to solutions containing either NO ₃ ^– or Cl^– to replace SO ₄ ^2– . The hyperpolarizations produced by Cl^– depend on external pH, being smaller in acid than in alkaline solutions. By contrast, hyperpolarizations produced by NO ₃ ^– were independent of external pH over a pH range from 5.5 to 9.0.In addition, voltage-clamp measurements were made on short lumbricalis muscle fibers. Initially they were equilibrated in isotonic solutions containing mainly K₂SO₄ plus Na₂SO₄. KCl or KNO₃ were added to the sulfate solutions and the fibers were equilibrated in these new solutions. When finally equilibrated the fibers had the same volume they had in the sulfate solutions before the additions. Constant hyperpolarizing voltage pulses of 0.6-sec duration were applied when all external K⁺ was replaced by TEA⁺. For these conditions, inward currents flowing during the voltage pulses were largely carried by Cl^– or NO ₃ ^– depending on the final equilibrating solution. Cl^– currents during voltage pulses were both external pH and time dependent. By contrast, NO ₃ ^– currents were independent of both external pH and time.The voltage dependence of NO ₃ ^– currents could be fit by constant field equations with aP _{NO 3} of 3.7·10^–6 cm/sec. The voltage dependence of the initial or instantaneous Cl^– currents at pH 7.5 and 9.0 could also be fit by constant field equations with P_Cl of 5.8·10^–6 and 7.9·10^–6 cm/sec, respectively. At pH 5.0, no measurable instantaneous Cl^– currents were found.From these results we conclude that NO ₃ ^– does not pass through the pH, time-dependent Cl^– channels but rather passes through a distinct set of channels. Furthermore, Cl^– ions do not appear to pass through the channels which allow NO ₃ ^– through. Consequently, the measured ratio ofP _Cl/P _{NO 3} based on membrane potential changes to ionic changes made on intact skeletal muscle fibers is not a measure of the selectivity of a single anion channel but rather is a measure of the relative amounts of different channel types.     

Microscopical determination of the filtration permeability of the mucosal surface of the goldfish intestinal epithelium

Summary The rate of shrinkage of the mucosal folds of goldfish intestine in response to mucosal hypertonicity was measured by microscopic means. Because of the geometry of the intestinal folds the rate of shrinkage could be directly related to the loss of volume from the fold through the brush border membranes and tight junctions. Experimentally a wide range of velocities was observed, reflecting the difficulty of rapidly estabilishing a uniform osmotic gradient at the preparation's mucosal surface. The initial velocity of volume loss provided a measure of the filtration permeability (P _f ) of the mucosal surface. From the highest velocities observed the filtration permeability was estimated to be approximately 14×10^–3 cm/sec related to the folded mucosal surface and 65×10^–3 cm/sec related to the straight serosal surface. Consideration of the experimental errors and unstirred layer effects make it probable that the latter value is still an underestimate of the trueP _f . The series barriers of the epithelium cause the total tissueP _f to be less than theP _f of the mucosal surface alone. In addition theP _f measured in the presence of an osmotic gradient may differ substantially from the tissue filtration permeability which exists in the absence of a change in osmolarity.     

Energy transfer to the reaction centres in bacterial photosynthesis

From a combined study of (1) bacteriochlorophyll fluorescence lifetimes, (2) relative yields and (3) differential absorption changes corresponding to the reaction centres photooxidation, the absolute values of fluorescence lifetimes and quantum yields for two bacteriochlorophyll fractions have been calculated. The main bacteriochlorophyll fraction (80–90%) serving as a light-gathering antenna for reaction centresP ₈₉₀ is characterized by dark values of fluorescence lifetimes of the order of 10^–11 sec and fluorescence yields of 10^–3. The remaining part of the bulk pigment, not associated withP ₈₉₀ as far as excitation energy transfer is concerned, has an approximately constant fluorescence yield of about 5–8% and lifetime of about 10^–9 sec. Basing on these results, excitation jump times and intermolecular coupling energies were estimated to be 10^–13 sec and 10^–2 ev respectively. The conclusion is made that excitation energy transfer in the main part of bacteriochlorophyll occurs by the exciton mechanism at moderate intermolecular energies.     

Effect of temperature on nonelectrolyte permeation across the toad urinary bladder

Summary The permeability of the toad urinary bladder to 22 nonelectrolytes was obtained from measurements of radioactive tracer fluxes. The permeability coefficients (P's), after suitable corrections for unstirred layers, were proportional to the olive oil/water partition coefficients for the majority of the molecules (P K_oil ^1.3). In the absence of chain branching, inductive effects, and intramolecular hydrogen bonding effects, a hydroxyl group reducedP an average 500-fold and a methylene group increasedP an average four fold. Branched chain solutes were less permeable than their straight chain isomers, and small solutes, polarand nonpolar, exhibited higher rates of permeation than expected from the relationship betweenP and K_oil. (Over the molecular size range 18–175 cc/moleP (Molecular Volume)^–2.7.) The high rates of permeation of small molecules are consistent with diffusion through a highly organized lipid structure. Large polar solutes, e.g., sucrose, appear to pass across the epithelium via an extracellular shunt pathway. The apparent activation energies (E _a ) for the permeation of 16 select molecules were obtained from permeability measurements over the temperature range 2–32°C. Linear Arrhenius plots (i. e., logP/T ^–1) were obtained for all molecules after unstirred layer corrections. In the absence of these corrections phase transitions were seen for molecules with very highP's (P>300×10^–7 cm/sec), but these are simply due to diffusion limited permeation.E _a increased by 2.5–3.6 kcals/mole with the introduction of each additional methylene group into a molecule, and decreased by up to 9 kcals/mole for the addition of a hydroxyl group. Qualitatively similar results were obtained in preliminary studies of olive oil/water partition coefficients. Arrhenius plots of the toad bladder conductance over the temperature range 2–32°C yield apparent activation energies of 4–5 kcals/mole which is identical to that found previously for leaky epithelia.     

Cation permeability ratios of sodium channels in normal and grayanotoxin-treated squid axon membranes

Summary Permeabilities of squid axon membranes to various cations at rest and during activity have been measured by voltage clamp before and during internal perfusion of 4×10^–5 m grayanotoxin I. The resting sodium and potassium permeabilities were estimated to be 6.85×10^–8 cm/sec and 2.84×10^–6 cm/sec, respectively. Grayanotoxin I increased the resting sodium permeability to 7.38×10^–7 cm/sec representing an 11-fold increase. The potassium permeability was increased only by a factor of 1.24. The resting permeability ratios as estimated by the voltage clamp method before application of grayanotoxin I were Na (1): Li (0.83): formamidine (1.34): guanidine (1.49): Cs (0.87): methylguanidine (0.86): methylamine (0.78). Grayanotoxin I did not drastically change the resting permeability ratios with a result of Na (1): Li (0.95): formamidine (1.27): guanidine (1.16): Cs (0.47): methylguanidine (0.72): methylamine (0.46). The membrane potential method gave essentially the same resting permeability ratios before and during application of grayanotoxin I if corrections were made for permeability to choline as the cation substitute and for changes in potassium permeability caused by test cations. The permeability ratio choline/Na was estimated to be 0.72 by the voltage clamp method and 0.65 by the membrane potential method. Grayanotoxin I decreased the ratio to 0.43. The permeability ratios during peak transient current were estimated to be Na (1): Li (1.12): formamidine (0.20): guanidine (0.20): Cs (0.085): methylguanidine (0.061): methylamine (0.036). Thus the sodium channels for the peak current are much more selective to cations than the resting sodium channels. It appears that the resting sodium channels in normal and grayanotoxin I-treated axons are operationally different from the sodium channels that undergo a conductance increase upon stimulation.     

Electrophysiological studies of pyridine-sensitive units on the crayfish walking leg

Summary Pyridine-sensitive units located on the walking legs of the crayfishAustropotamobius torrentium were studied by extracellular recording of the action potentials of single afferent fibers. To characterize the sensitivity and specificity of the pyridine receptor, 79 pyridine analogs and other related substances were tested on 70 neurons. The maximum impulse frequency of the response was used to construct dose-response curves. The effectiveness of stimulatory substances was characterized at the half-maximal-response frequency, K_M. The effectiveness rank order of the substances was found to be the same for all units tested. The most effective substances were: pyrazinecarboxamide > 3-acetylpyridine > nicotinamide > pyridine-3-aldoxime, with K_M values of 1.5×10^–6, 4× 10^–6, 10^–5 and 4 x 10^–5 mol/1, respectively. The inferred structural requirements for an optimal stimulatory molecule are that it have a N-containing aromatic ring system with a specific substituent in them position.     

Electrogenic and diffusive components of the membrane ofHydrodictyon africanum

Summary In cells of the freshwater algaHydrodictyon africanum, in solutions where [K⁺]₀=0.1mm and pH₀>7.0, the membrane in the light is hyperpolarized. The membrane potential difference {ie179-1} has values from –180 to –275 mV, more negative than any ion diffusion potential difference, and is predominantly a function of pH₀, and independent of [K⁺]₀. The hyperpolarization of the membrane appears to arise from an electrogenic efflux of H⁺, estimated from voltage-clamp data to be about 8 nmol m^–2 sec^–1 when pH₀=8.5. In the light the membrane conductanceg _m is about 0.084 S m^–2. At light-off, {ie179-2} becomes less negative, with a halftime for change of 15 to 30 sec andg _m decreases by about 0.052 S m^–2. After dark periods of up to 300 sec, {ie179-3} is largely independent of pH₀ for values greater than 6.0 and usually behaves as a combined K⁺ and Na⁺ diffusion potential with permeability ratioP _Na/P _K=0.05 to 0.2. The membrane potassium conductanceg _K has either a low value of 2–6×10^–2 Sm^–2, or a high value of up to 18×10^–2 S m^–2 depending on [K⁺]₀, the transition from low to high values occurring when {ie179-4} moves over a threshold value that is more negative than {ie179-5}, the electrochemical equilibrium potential for K⁺. The time for half-change of the transition is about 30 sec. The results are consistent with a model of the membrane in which the pump electromotive force and conductance are in parallel with diffusive electromotive forces and conductances. When the pump is operating its properties determine membrane properties, and when it is inoperative, or running at a diminished rate, the membrane properties are determined more by the diffusive pathways. Changes in both pump rate andg _K can account for a variety of characteristic changes in membrane PD and conductance occurring in response to ligh-dark changes, changes in light intensity, pasage of externally applied electric current across the membrane and changes in ionic constituents of the external medium.     

Independence of water and solute pathways in human RBCs

We have investigated the permeability of the human red blood cell to four di-hydroxy alcohols, 1,2PD (1,2 propanediol), 1,3PD (1.3 propanediol), 1,4BD (1,4 butanediol), and 2,3BD (2,3 butanediol), and to water by using a recently developed ESR stopped-flow method which is free from artifacts found in light scattering methods. Numerical solutions of the Kedem-Katchalsky equations fit to experimental data yielded the following permeability coefficients: P_1,2PD = 3.17 × 10^–5 cm sec^–1, p_1,3pd = 1.75 × 10^–5 cm sec^–1, P_1,4BD = 2.05 × 10⁵ cm sec^–1, P_2,3BD = 7.32 × 10^–5 cm sec^–1. Reflection coefficients () were evaluated by comparing data fit with assumed values of = 0.6,0.8 and 1.0. In all four cases the best fit was obtained with = 1.0. Treatment of cells with PCMBS (para-chloro mercuri-benzenesulfonate) was followed by a large (> 10-fold) decrease in water permeability with virtually no change in alcohol permeability. We conclude that these alcohols do not permeate the water channels to any significant extent, and discuss some of the problems in light scattering measurements of reflection coefficients that could lead to erroneous values for .We would like to thank Professor Lenore W. Yousef (Dept. of Biology, California State Univ., Fresno) for valuable discussions and critical comments. We thank Lidia Mannuzzu for measurements of ESR spectra in the presence and absence of alcohol. We are also indebted to Kate Van Fossen for her dedicated technical support. This work was supported by NIH grant No. HL-20985.     

Photon correlation spectroscopy of human IgG

The translational diffusion coefficient D _20,w ⁰ , of monomeric human immunoglobulin G (IgG) has been studied by photon-correlation spectroscopy as a function of pH and protein concentration. At pH 7.6, we find D _20,w ⁰ =3.89×10^–7±0.02 cm²/sec, in good agreement with the value determined by classic mehods. This value corresponds to an effective hydrodynamic radius R, of 55.1±0.3 Å. As pH is increased to 8.9; with the same ionic strength, the molecule appears to expand slightly (3.5% increase in hydrodynamic radius). The concentration dependence of the IgG diffusion constant is interpreted in terms of solution electrostatic effects and shows that long-range repulsive interactions are negligible in the buffer used. The diffusion coefficient for dimeric IgG has also been determined to be D_20,w=2.81×10^–7±0.04 cm²/sec at 1.6 mg/ml, which corresponds to a hydrodynamic radius of 75 Å. For light-scattering studies of protein molecules in the dimension range of 5–10 nm (M_r=10⁵–10⁷) we find monomeric horse spleen ferritin well suited as a reference standard. Ferritin is a spherical molecule with a hydrodynamic radius R of 6.9±0.1 nm and is stable for years in our standard Tris-HCl-NaCl buffer even at room temperature.     

Size selectivity of aqueous pores in astomatous cuticular membranes isolated from<Emphasis Type="Italic"> Populus canescens</Emphasis> (Aiton) Sm. leaves

Little is known about the permeability of plant cuticles to ionic molecules with hydration shells that render them lipid insoluble and limit their diffusion to narrow aqueous pores. Therefore, the permeation of cuticular membranes to ionised calcium salts with anhydrous molecular weights ranging from 111 to 755 g mol^–1 was studied. Penetration was a first-order process and rate constants (k) (proportional to permeability) decreased exponentially with molecular weight. Plots of log k vs. molecular weight had slopes of –2.11×10^–3 and –2.80×10^–3, respectively, depending on the year in which the cuticular membranes were isolated. This corresponds to decreases in permeability by factors of about 7 to 13 when molecular weight increased from 100 to 500 g mol^–1. This size selectivity is small compared to the dependence on molecular weight of solute mobility in Populus cuticles. A decrease in mobility of neutral molecules by more than 3 orders of magnitude has been reported [A. Buchholz et al. (1998) Planta 206:322–328] for the same range of molecular weights. Hence, discrimination of large ionic species diffusing in aqueous pores (polar pathway) is much smaller than that for neutral solutes diffusing in cutin and waxes (lipophilic pathway). This indicates that formulating large solutes as ionic species would be advantageous.Abbreviation CM Cuticular membrane     

Cheek cell membrane fluidity measured by fluorescence recovery after photobleaching and steady-state fluorescence anisotropy

Membrane fluidity of human cheek cells was determined using fluorescence recovery after photobleaching (FRAP) and steady-state fluorescence anisotropy. The FRAP data showed that the lateral diffusion coefficient (D) and mobile fraction (%R) of lipid in the plasma membrane of control cells were 2.01×10^–9 cm²/ sec and 54.25%, respectively. Trypsin treatment increased D and %R to 6.4×10^–9 cm²/sec and 72.15%. In contrast, the anisotropy (r) for control cells was 0.270 which remained unchanged by trypsin treatment. The results show that diffusion of lipids in the plane of the membrane is restricted by trypsin-sensitive barriers.