Diffusion of bacteriophages through artificial biofilm models

The simple two-chamber diffusion method was improved to study the diffusion properties of bacteriophage (phage) T4 through a model biofilm agarose gel membrane (AGM) embedded with dead host Escherichia coli K12 cells. The apparent diffusion coefficient (D(app) ) of phage T4 was calculated to be 2.4 × 10(-12) m(2) /s in 0.5% AGM, which was lower than the coefficient of 4.2 × 10(-12) m(2) /s in 0.5% AGM without host cells. The phage adsorption process by dead host cells slowed the apparent phage diffusion. The Langmuir adsorption equation was used to simulate phage adsorption under different multiplicity of infections (MOIs); the maximum adsorbed phage MOI was calculated to be 417 PFU/CFU, and the Langmuir adsorption constant K(L) was 6.9 × 10(-4) CFU/PFU. To evaluate the effects of phage proliferation on diffusion, a simple syringe-based biofilm model was developed. The phage was added into this homogenous biofilm model when the host cells were in an exponential growth phase, and the apparent diffusion coefficient was greatly enhanced. We concluded that D(app) of phages through biofilms could be distinctly affected by phage adsorption and proliferation, and that the idea of D(app) and these methods can be used to study diffusion properties through real biofilms.     

Transduction of a Plasmid with an Inserted R4 Phage DNA Fragment in Streptomyces lividans

A Streptomyces plasmid, pR4C2, with an inserted DNA fragment of R4 phage, was encapsidated into R4 phage particles in vivo and transduced to Streptomyces lividans at 3 ×10^?6CFIJ/PFU. Formation of transducing phage was dependent on the inserted R4 DNA, and some of the transducing phages had larger DNA than R4 phage. A possible transduction mechanism through plasmid-phage cointegrate formation in vivo is discussed.     

Transient electric birefringence of the bacteriophages T3 and T7

Electric birefringence measurements of suspensions of T3 and T7 bacteriophages in 10^?2 M phosphate buffer, pH 6.9, show that there is a difference in their rotational diffusion coefficient. The values corrected to 25°C and water viscosity are D_25,w = 4630 ± 130 sec^?1 and D_25,w = 5290 ± 260 sec^?1 for T3 and T7, respectively. The value obtained from shell model calculations (according to Filson and Bloomfield) is D_25,w = 4500 ± 600 sec^?1. The apparent permanent dipole moments are 4.5 × 10^?26 C·m and 1.7 × 10^?26 C·m for T3 and T7, respectively. For both phage particles the intrinsic optical anisotropy is +7.2 × 10^?3. It is shown that this anisotropy is mainly due to the DNA molecule inside the head of the phage. Its positive value means that there exists an excess orientation of the DNA helix perpendicular to the symmetry axis of the particle. For T7 an unexpectedly large increase of Δn_s and K_sp occurs at a glycerol concentration of about 30% (v/v). This increase is interpreted as being caused by a change of the shape of the particle and/or a change in the secondary structure of the DNA inside the head of the bacteriophage.     

Combined treatment of Pseudomonas aeruginosa biofilms with bacteriophages and chlorine

Bacterial biofilms are a growing concern in a broad range of areas. In this study, a mixture of RNA bacteriophages isolated from municipal wastewater was used to control and remove biofilms. At the concentrations of 400 and 4 × 10⁷ PFU/mL, the phages inhibited Pseudomonas aeruginosa biofilm formation by 45 ± 15% and 73 ± 8%, respectively. At the concentrations of 6,000 and 6 × 10⁷ PFU/mL, the phages removed 45 ± 9% and 75 ± 5% of pre‐existing P. aeruginosa biofilms, respectively. Chlorine reduced biofilm growth by 86 ± 3% at the concentration of 210 mg/L, but it did not remove pre‐existing biofilms. However, a combination of phages (3 × 10⁷ PFU/mL) and chlorine at this concentration reduced biofilm growth by 94 ± 2% and removed 88 ± 6% of existing biofilms. In a continuous flow system with continued biofilm growth, a combination of phages (a one‐time treatment at the concentration of 1.9 × 10⁸ PFU/mL for 1 h first) with chlorine removed 97 ± 1% of biofilms after Day 5 while phage and chlorine treatment alone removed 89 ± 1% and 40 ± 5%, respectively. For existing biofilms, a combined use of a lower phage concentration (3.8 × 10⁵ PFU/mL) and chlorination with a shorter time duration (12 h) followed by continuous water flushing removed 96 ± 1% of biofilms in less than 2 days. Laser scanning confocal microscopy supplemented with electron microscopy indicated that the combination treatment resulted in biofilms with lowest cell density and viability. These results suggest that the combination treatment of phages and chlorine is a promising method to control and remove bacterial biofilms from various surfaces. Biotechnol. Bioeng. 2013; 110: 286–295. © 2012 Wiley Periodicals, Inc.     

Dynamic light scattering from thin rigid rods: Anisotropy of translational diffusion of tobacco mosaic virus

An Exact theoretical expression for the apparent diffusion coefficient D_app(K) of a thin rigid rod with arbitrary anisotropy of its translational diffusion diffusion coefficient is derived from the first cumulant of its dynamic structure factor. D_app(K) is predicted to reach a limiting plateau value at extermely large values of KL, where K is the scattering vector and L the rod length. Howerver, that limiting plateau value is approached only very slowly along a quasi-plateau with a very gradual slope. Dynamic light-scattering studies have been performed on tobacco mosaic virus from K² = (0.4–20) × 10¹⁰ cm^?2 using 632-8-nm laser radiation. The present data yield D₀ = (4.19 ± 0.10) × 10^?8 cm²/s (corrected to 20,w conditions) and, with literature data to establish L = 2980 Å and the rotational diffusion coefficient D_R = 318s^?1, yield also Δ ≡ D_∥ ? D_⊥ = (1.79 ± 0.38) × 10^?8 cm²/s. The experimental data closely follow the curve of D_app(K) vs K² calcuated for these parameters. The present value of D₀ substantially exceeds all previous dynamic light-scattering values, but is in good aggreement with previous sedimentation data, which were confirmed for the presemt sample. The anisotropy ratio Δ/D₀ = 0.43 ± 0.09 is in accord with theoretical predictions based on the modified Kirkwood algorithm, despite the fact the D₀ lies significantly below its corresponding theoretical value. The present data largely predlude the possibility that both D₀ and Δ/D₀ could simultaneously match their theoretical predictions. We present a detailed comparison of the experimental data with the calculations of Tirado and Garcia de la Torre based on the modified Kirkwood algorithm and with the Broersma formulas.     

Dynamic light scattering of the bacteriophage T4B: determination of translational diffusion coefficients and centres of rotation

Using dynamic light scattering, the translational diffusion coefficient (D_T) and the distance between the hydrodynamic centre and the centre of the head (r₀) of the bacteriophage T4B have been determined. For a particle with retracted tail fibres we found D_T20.w =2.88 (2.88 ± 0.02) × 10^?8cm²s^?1 and r₀ = 52 ± 1 nm. For a phage with fully extended tail fibres D_T20w = (.210 ± 0.02) × 10^?8cm²s^?1 and r₀ = 112 ± nm. These data were obtained by interpreting the correlation function using a theory which takes into account the influence of the lollipop shape of the phage. In the literature this influence has not been taken into account, which has led to erroneous values of diffusion coefficients for T4B and other phages. The sedimentation coefficient of T4B phage is 1040 ± 5 S (fibres retracted) or 829 ± 4 S (fibres extended). With the above mentioned diffusion coefficients, these values correspond to a molecular weight of 236 × 10⁶ ± 3 × 10⁶. Finally, the theory used in this study is applied to other bacterial viruses, to correct reported values of the translational diffusion coefficients and of the corresponding molecular weights of these viruses.     

Measurement of diffusion coefficient and electrophoretic mobility with a quasielastic light-scattering–band-electrophoresis apparatus

We have constructed an apparatus for the simultaneous measurement of electrophoretic mobility, μ, and diffusion coefficient, D, of macromolecules and cells. It combines band electrophoresis in a vertical, sucrose-gradient stabilized column, with quasielastic laser light-scattering determination of the diffusion coefficient of the species within the band. The entire electrophoresis cell is scanned through the laser beam of the quasielastic laser light-scattering apparatus by a vertical translation stage. Total intensity light-scattering measurement at each point in the cell gives the macromolecular concentration at that point. Solvent viscosity and electrical potential are measured at each point in the cell. Application of this apparatus to resealed red blood cell ghosts and to bovine hemoglobin indicates that measurements of field, viscosity, and migration distance are reliable, and that electroosmosis is insignificant. Application to T4D bacteriophage gives μ_20,w = (?1.05 ± 0.05) × 10^?4 cm²/V sec and D_20,w = (3.35 ± 0.10) × 10^?8 cm²/sec for fiberless particles, and μ_20,w = ?(0.59 ± 0.03) × 10^?4 cm²/V sec and D_20,w = (2.86 ± 0.09) × 10^?8 cm²/sec for whole phage with 6 fibers. Approximate analysis of these results with the Henry electrophoresis theory for spheres in dicates that each fiber contributes about 193 positive charges to the phage particle, compared with 327 from amino-acid analysis. The advantages and disadvantages of this apparatus, relative to conventional electrophoresis and to electrophoretic light scattering, are discussed.     

Li+ counterion self-diffusion in ordered DNA

The anisotropic self-diffusion coefficient of ⁷Li⁺ (I = 3/2) counterions has been studied in hydrated, macroscopically oriented Li-(B)DNA fibers at relatively high water contents, corresponding to approximate DNA-DNA helix axis distances of 22–35 Å, using the pulsed field gradient hmr spin-echo method. Self-diffusion coefficients parallel (D_∥) and perpendicular (D_?) to the DNA helix axis increase with increasing salt content and with increasing DNA-DNA helix axis distance. The observed anisotropy D_∥/D_? decreases from 1.6 to 1.2 with the DNA-DNA separation increasing from 22 to 35 Å in the salt-free sample. This result can be understood by the obstruction effect caused by the DNA molecules themselves. The values of the Li⁺ self-diffusion coefficients in the most water-rich system with no added salt (corresponding to an approximate distance of 35 Å between the DNA helix axes) were D_∥ ～ 1.15 × 10^?10 m² s^?1 and D_? ～ 0.98 × 10^?10 m² s^?1, compared to 9.14 × 10^?10 m² s^?1 for the diffusion of Li⁺ in an aqueous solution of LiCl (～ 2.1M). The possible occurrence of restriction effects in the DNA fibers have also been studied by determining the self-diffusion coefficient at different effective diffusion times. The self-diffusion coefficient of Li⁺ in the sample with the largest DNA-DNA helix axis distance seems to be independent of the effective diffusion time, which indicates that the lithium ions are not trapped within impermeable barriers. The possibility of diffusion through permeable barriers has also been investigated, and is discussed. © 1994 John Wiley & Sons, Inc.     

Transient electric birefringence of T-even bacteriophages. IV. T2L0 and T6 with extended tail fibers

Transient electric birefringence measurements of the bacteriophages T2L0 and T6 were performed under such conditions that the tail fibers are extended. The data obtained are compared to previously reported data for T4B. For all T-even phages the degree of extension of the tail fibers is a function of pH, ionic strength, and temperature. For T4B, much higher ionic strengths are needed than for T2L0 and T6 to accomplish complete tail-fiber extension. The rotational diffusion coefficients of the phages with fully extended fibers are equal to 120 ± 3 sec^?1, 132 ± 5 sec^?1, 157 ± 4 sec^?1 for T2L0, T4B, and T6, respectively. The respective optical anistropies are ? (2.66 ± 0.05) × 10^?4, and ? (3.07 ± 0.15) × 10^?4. The differences in the rotational diffusion coefficient and optical anisotropy arise because the conformation of the fully extended tail fibers is different for the three phages. The tail fibers of T2L0 project further into the solution (away from the head) than do those of T4B and T6. The apparent permanent dipole moments of T2L0 and T6 decrease with increasing ionic strength. This decrease is caused by the screening of the surface charges on the phage body by the counter-ions in the solution. The biological relevance of this decrease is illustrated by the fact that the adsorption rate of T6 phages to E. coli B bacteria shows a similar dependence of ionic strength. Evidence is pressented that the tail fibers may move more or less independently of the phage body when an electric field is applied to the suspension.     

Bacteriophages of l-Glutamic Acid-Producing Bacteria

The growth characteristics of phages were investigated with the four phages, active on Brevibacterium lactofermentum, which were selected from the respective serological groups, namely, P465 (group I), P468II (group II), Ap85III (group III) and P4 (group IV).

The adsorption rate of the phages, P465 and P468II, on the host bacteria was low, whereas that of the phages, Ap85III and P4, was higher. The adsorption rate constants for the four phages were respectively calculated at 2.02 × 10^?10, 1.87 × 10^?10, 4.32 × 10^?10 and 3.15 × 10^?10 cm³ per minute, at 30°C in G₅B₂ medium. With reference to the ionic environment for adsorption, the phages, P465 and Ap85III, specifically required either for Ca⁺⁺ or Mg⁺⁺; the phage P468II, for both; and the phage P4, for neither.

The growth characteristics of these phages were examined by the one-step growth experiment. The latent periods of the phages were 50, 53, 57 and 47 minutes, respectively; and the corresponding average burst sizes were about 98, 31, 145 and 126. The growth of the phage P4 was completely suppressed at above 34°C, although the host bacteria and the other three phages were capable of the full growth at that temperature.     

High-frequency transduction of pBR322 by cytosine-substituted T4 bacteriophage: evidence for encapsulation and transfer of head-to-tail plasmid concatemers

Transduction of plasmid pBR322 by cytosine-substituted T4 phages has been studied. Three T4 phage mutants which substitute cytosine for all of hydroxymethylcytosine residues in the DNA, were shown to transduce pBR322 at frequencies of 2 × 10^?2 to 4 × 10^?3 transductants per singly infected cell. Also, three T4 phage strains which partially substitute cytosine for hydroxymethylcytosine, transduced pBR322 at frequencies of 2 × 10^?3 to 2 × 10^?4. The transduction frequencies of pBR322 we attained are at least 10-fold higher than those reported by G. G. Wilson, K. Young, and G. J. Edlin (1979, Nature (London)280, 80–82). We found that multiplicity of infection in preparation of the transducing phage is the most important factor affecting the frequency of pBR322 transduction. When a lysate made at a multiplicity of infection ranging from 0.5 to 0.05 was used as the donor phage, transduction frequency of pBR322 was 10- to 40-fold higher than that of high-m.o.i. lysate. The transduction frequency was not affected by either restriction systems or amber suppressors of the recipient cells. However, no pBR322-containing transductant was obtained when either recA or polA mutants were used as the recipients. DNA from T4dC phage containing pBR322-transducing particles was analyzed on agarose gel electrophoresis after cleavage with restriction endonucleases. It was suggested that the pBR322 DNA in the T4dC phage particles exists as head-to-tail concatemers.     

Transient electric birefringence of T-even bacteriophages. II. T4B in the presence of tryptophan and T4D.

Measurements of electric birefringence, sedimentation velocity, and biological adsorption rate are used to study the properties of bacteriophage T4B in the presence of excess tryptophan. The adsorption rate determined in borate buffer pH 9 (at 25°C) increases from 0.003 × 10^?8 ml min^?1 (0.025 M) to 0.130 × 10^?8 ml min^?1 (0.150 M). The Kerr coefficient, rotational diffusion coefficient, and the sedimentation coefficient of the phage are also dependent on buffer concentration and reach plateau values above 0.12 M given by K_sp = ?(275 ± 18) × 10^?9 OD^?1 cm² statvolt^?2, D_25,w = 133 ± 4 sec^?1, and s_20,w = 818 ± 11 S. From a comparison of electric birefringence measurements of T4B and T4D it is concluded that T4D and T4B (in the presence of excess tryptophan) exhibit a similar hydrodynamic behavior. The change in physical parameters is solely due to a shift in fiber configuration. At high buffer concentrations the fibers make an angle of approximately 3π/4 with the sheath and the permanent dipole moment is about 200,000 D. This dipole moment is roughly ten times as large as that of a phage particle with nonextended fibers. This difference may be due to a change in hydrodynamic center upon fiber extension or to the presence of positive charges on the fiber tips, or both. At intermediate buffer concentrations the phage population behaves as if it were monodisperse. Probably not all six fibers are extended under such conditions.     

Histone-induced conformational changes in DNA as probed by quasi-elastic light scattering.

Quasi-elastic light scattering as measured by intensity fluctuation (self-beat) spectroscopy in the time domain can be profitably used to follow both the translational diffusion D and the dominant internal flexing mode τ_int of DNA and its complexes with various histones in aqueous salt solutions. Without histones, DNA is found to have D = 1.6 × 10^?8 cm²/sec and τ_int ? 5 × 10^?4 sec in 0.8 M NaCl, 2 M urea at 20°C. Total histone as well as fraction F2A induce supercoiling (D = 2.6 × 10^?8 cm²/sec, τ_int ? 2.8 × 10^?4 sec) whereas fraction F1 induces uncoiling (D = 1.0 × 10^?8 cm²/sec, τ_int ? 9.4 × 10^?4 sec). Upon increasing the salt concentration to 1.5 M the DNA–histone complex dissociates (D = 1.8 × 10^?8 cm²/sec). Upon decreasing the salt concentration to far below 0.8 M, the DNA–histone complex eventually precipitates as a chromatin gel.     

Dynamic light scattering from collagen solutions. I. Translational diffusion coefficient and aggregation effects

Solutions of native collagen extracted from rat tail tendons in neutral salt solution have been studied by dynamic light scattering. The spectra obtained are consistent with the presence in solution of both single rod-shaped collagen molecules and aggregates of molecules. No contribution to the spectrum has been detected at any scattering angle from rotational diffusion of single molecules, although a measurable broadening effect is expected at high angles. The translational diffusion coefficient D of single molecules, calculated from the broader spectral component, shows an anomalous dependence on collagen concentration with a maximum value of D_20,w = 8.6 ± 0.2 × 10^?12 m²/sec near the concentration 0.04% by weight. Above 0.05% D falls linearly with increasing concentration and takes the value D _20,w = 8.1 ± 0.2 × 10^?12 m²/sec at 0.064% collagen.     

The titratable joint phenomenon in ΦW-14 DNA

Dynamic light scattering (DLS) studies are carried out on native ΦW-14 DNA, which has putrescines covalently attached at the methyl groups of half its thymines, and on a chemically modified form of the same DNA in which the ammonium groups of its putrescines are almost completely acetylated. From neutrality to pH 9.6, both forms of ΦW-14 DNA exhibit the same curve of D_app vs K² over the range K² = 0.5 × 10¹⁰ to K² = 20 × 10¹⁰ cm^?2, and this coincides with curves that we have observed for other DNAs. (D_app, apparent diffusion coefficient; K, scattering vector). However, when the pH is raised to pH 10.0–10.2, native ΦW-14 exhibits a spectacular decrease in D_app at large wave vector, whereas the acetylated form shows no sign of such behavior. It is inferred that bound ammonium groups make an essential contribution to the stabilization of titratable joints. Comparing the pH profiles of the absorbance (A₂₆₀) for these two DNAs gives some evidence that base unstacking may be involved in titratable joint formation.     

EAEC噬菌体PNJ1809-11和PNJ1809-13作为环境消毒剂的杀菌效果评估

[目的]分析2株肠聚集性大肠杆菌(EAEC)CVCC232噬菌体PNJ1809-11、PNJ1809-13的生物学特性,并对其作为环境消毒剂的杀菌效果进行评估.[方法]透射电镜下观察PNJ1809-11、PNJ1809-13的形态;通过宿主谱、最佳感染复数(MOI)、一步生长曲线、对pH和温度耐受性的测定分析PNJ18...     

Translational and rotational diffusion of tobacco mosaic virus from polarized and depolarized light scattering

The translational and rotational dynamics of tobacco mosaic virus in sodium phosphate buffer (pH =7.5) solutions has been investigated by polarized and depolarized light scattering Rayleigh linewidth studies. For concentrations ranging from 1.75 × 10^?4 g ml^?1 to 0.25 × 10^?4 g ml^?1 the translational diffusion coefficient (D_T) has been found to be slightly concentration dependent and extrapolation to zero concentration gives D₀^20°C = 0.34 ± 0.01 × 10^?7 cm²S^?1. A full analysis of the polarized spectra obtained at high and low scattering angles and the depolarized spectra at near zero scattering angles has enabled these techniques to be compared and the rotational diffusion constant D_R to be determined. At a solution concentration of 1.75 × 10^?4 g ml^?1 a mean value is found to be D_R^20°C = 350 ± 30s^?1. These values of D_T and D_R are in approximate agreement with calculations based on models of the tobacco mosaic virus molecule as a cylindrical rod.     

Phage display screening of TIGIT-specific antibody for antitumor immunotherapy

ABSTRACT

The fully synthetic humanized phage antibody library has the advantages including the minimized immunogenicity, which frequently happened in hybridoma cell-based antibody production. In this paper, using the constructed diverse complementarity determining region gene library and the germline gene as the backbone, we constructed eight single-chain antibody libraries and a combinatorial antibody library with a big capacity of 1.41 × 10¹⁰. M13EEA helper phage that was engineered from M13KO7 was applied to prepare phage antibody library. The eukaryotic expression of T-cell immune receptor with Ig and ITIM domain (TIGIT) antigen was used as a target antigen for screening. The screening of antigen-specific single-chain Fc-fused protein was performed through evaluation of binding affinity based on ELISA analysis. The IgG antibody was prepared with the screened single-chain protein. Finally, the CB3 antibody was screened out which exhibits the highest binding affinity with TIGIT with the K_d value of 8.155 × 10^?10 M.     

Boundaries of the universal K3 region and plateau region of the dynamic structure factor for DNA

A sufficiently long semiflexible filamentous macromolecule is theroretically expected to exhibit three different domains of behavior of its apparent diffusion coefficient D_app(K) as a function of scattering vector K: (1) the small wave vector limit, where D_app(K) = D₀ is the translational diffusion coefficient of the center-of-mass; (2) the universal K³ region, where D_app(K) = (k_BT/6πη)K is a universal function of K independent of any property of the molecule itself; (c) the plateau region at large K², where D_app(K) approaches either a plateau, or gradually sloping quasiplateau, characteristic of local (elastic) rigid-body motions of the filament. The existence of each of these different domains has now been established experimentally for at least some polymers. The boundaries of the universal K³ region and the plateau region are determined theoretically here using precise quantitative criteria for universal or plateau behavior of D_app(K) for a Rouse-Zimm model containing N + 1 subchains with rms subchain extension b. Allowing a maximum of 13% nonuniversal behavior, the domain of the universal K³ region is given by K²R²_G = K²Nb²/6 ≥ 7 and K²b² ? 0.54. Allowing as much as 10% nonplateau behavior, the boundary for onset of plateau behavior is K²b² = 18.3. D_app(K) is at least 50% nonuniversal when K²b²/6 = 6 ln 3. Extension of these results to DNA is examined theoretically, and good agreement of the pertinent predictions with published experimental data is demonstrated. It is concluded that no truly universal K³ region exists for DNA with M_r ? 10⁷ and persistence length a ≥ 450 Å, although marginally (?17% nonuniversal) universal behavior, is exhibited in a very narrow domain 0.64 × 10¹⁰ ? K² ? 0.84 × 10¹⁰ cm^?2 for ?29 DNA (M_r = 11.5 × 10⁶). More than 50% of D_app(K) is governed by local (elastic) rigid-body motions when K² = 5.23 × 10¹⁰ cm^?2. The existence of a very wide region of nonuniversal apparent K³ behavior extending up to very large K², far into the plateau region, is demonstrated in a plot of D_app(K)/K vs K² for the Rouse-Zimm model. This is shown to stem in part from visual artifacts of plotting D_app(K)/K vs K², even for rigid species.     

Purification and Properties of 2-Ketogluconate Reductase from Gluconobacter liquefaciens.

2-Ketogluconate reductase (2KGR) from the cell free extract of Gluconobacter liquefaciens (IFO 12388) was purified about 1000-fold by a procedure involving ammonium sulfate fractionation and column chromatographies using DEAE-cellulose, hydroxylapatite, and Sephadex gel The purified enzyme gave a single band on polyacrymamide gel electrophoresis. NADP was specifically required for the oxidation reaction of gluconic acid. Using gel filtration a molecular weight of about 110,000 was estimated for the enzyme. The pH optimum for the oxidation of gluconic acid (GA) to 2-ketogluconic acid (2KGA) by the enzyme was 10.5 and for the reduction of 2KGA was 6.5. The optimum temperature of the enzyme was 50 C for both reactions of oxidation and reduction. The enzyme was stable at pH between 5.0 and 11.0 and at temperature under 50°C, The enzyme activity was strongly inhibited with p-chloromercuribenzoate and mercury ions, but remarkably stimulated by manganese ions (1×10^?3 m). Km value of the enzyme for GA was 1.3×10^?2 m and for 2KGA was 6.6×10^?3 _m. Km values for NADP and NADPH₂ were 1.25×10^?5 and 1.52×10^?5 m respectively.