Plasminogen activator secretion during mouse embryogenesis.
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Biomedical subjects
Publications and source records attributed to V C Bode.
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The biological containment of the lambda gt family of cloning vectors has been enhanced by conditionally blocking DNA replication as well as head and tail morphogenesis. The vector, lambda gtALO.lambda B, was constructed by crossing the Oam29, Aama1 and Lam439 mutations into lambda gt.lambda B. The mutation blocking phage DNA replication, Oam29, is suppressed by suII+ or suIII+. The head gene mutation, Aama1, is suppressed by suIII+ but not by suII+ and the tail gene mutation, Lam439, is suppressed by suII+ but not by suIII+. This allows the option of increasing the biological containment by producing heads when a large amount of cloned DNA is being prepared from an individual isolate. A model recombinant, lambda gt Aama1 Lam439 Oam29.KmR' (lambda gtALO.KmR') was constructed and the containment of the vector was evaluated by the series of standardized experiments required for EK2 certification.
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Ethidium-binding isotherms for purified circular lambda DNA, isolated from a superinfected lysogen, and for linear lambda DNA, isolated from the purified phage, were constructed from fluorescence measurements of ethidium-DNA MIXTURES. The measurements were made in 0.01 M Tris-HC1-0.001 M EDTA,pH 7.1, buffer at 20 degrees and in the same buffer containing 0.1, 0.4, or 1.0 M NaC1. When NaC1 was present, differences in the binding affinity for supercoiled and linear DNA could be quantitated. As the ethidium concentration was increased, supercoiled lambda DNA molecules bound the intercalating dye first more and then less avidly than nonsupercoiled ones. The number of potential supercoils in a circular lambda DNA molecular in the absence of dye was calculated from the amount of dye bound when it exhibited the same affinity for dye as its linear counterpart. The point of equivalent affinity shifted from 0.053 mol of dye bound per mol of nucleotide in 0.1 M NaC1 to 0.067 mol in 1.0 M NaC1. This corresponds to the removal of 164 and 206 supercoiling turns per molecule and superhelix densities in the absence of dye equal to 0.036 and 0.045 superhelical turns per 10 base pairs. If this difference in the number of supercoils reflects a salt-dependent change in the average rotation angle between base pairs of the Watson-Crick helix the angle differs by 0.32% in the two ionic environments.
The sedimentation of circular lambda DNA suggests that the molecular undergoes significant changes in shape and super-coiling as the NaC1 concentration increases. Closed circular lambda DNA, species I, isolated and purified from superinfected immune bacteria, sediments in sucrose gradients of low ionic strength at a rate 2.0 times faster than linear lambda DNA, species III. The addition of ethidium causes the sedimentation rate of species I DNA to decrease until enough dye is bound to remove 121 supercoils per molecule. At this point, species I co-sediments with nicked and nonsupercoiled species II. Futher additions of ethidium cause the sedimentation rate to increase until the relative rate of species I is again at least twice that of species III. This classical behavior is altered when NaC1 is present in the buffer. In 1.0 M NaC1 the changes in S are complex. Initially, species I sediments 1.55 times faster than species III. Titration with ethidium caused a decrease in S to an early minimum value, than an increase to a first maximum, followed by a decrease to the S of species II. At this point enough dye has intercalated to remove 208 superhelical turns. Further additions of dye introduce supercoils and cause S to increase again. In 0.1 to 0.4 M NaC1 the relative S of species I is 1.69 and 1.59, respectively. If titrated with ethidium, S first increases to a maximum value then decreases to the minimum rate when enough dye is bound to remove 158 and 183 supercoils, respectively. The results indicate an increase in the superhelix density from 0.026 turns per 10 base pairs in buffer alone to 0.045 in the same buffer with 1.0 M NaC1. If this change in superhelix density results from a concomitant change in the average rotation angle between base pairs in the Watson-Crick helix, the addition of 1.0 M NaC1 alters the rotation angle by 0.68 degrees per base pair.