Penicillin-binding proteins in Bacillus subtilis mutants

The penicillin-binding proteins (PBPs) from mutants of Bacillus subtilis were studied and related to morphology. In a previously described cloxacillin-resistant mutant of B. subtilis strain Porton, PBP 2a had an altered mobility by sodium dodecyl sulfate gel electrophoresis and was present in increased amounts. In addition, PBPs 1a and 1b were missing in this mutant. The only morphological change seen was a decrease in size of about 15%. Studies of two Triton-resistant morphological mutants of B. subtilis 168, Tr49 (small diameter) and Tr61 (helical form), revealed no change in the number of PBPs compared with that of the parent strain. However, PBPs 1a and 1b had an altered mobility in the mutant Tr49.

Linear, uncross-linked peptidoglycan secreted by penicillin-treated Bacillus subtilis. Isolation and characterization as a substrate for penicillin-sensitive D-alanine carboxypeptidases

Incubation of growing Bacillus subtilis with penicillin G led to the secretion of a peptidoglycan-related polymer and a nonglycan-bound pentapeptide into the culture medium. The secreted polymer was isolated and characterized as a linear cell wall glycan strand substituted predominantly by uncross-linked pentapeptide side chains. Polymer formation and secretion are most likely the result of continued synthesis and elongation of nascent glycan strands in the absence of subsequent processing by peptidoglycan transpeptidase or D-alanine carboxypeptidase enzymes. The nonglycan-bound pentapeptide, L-Ala-D-iso-Glu-meso-diaminopimelic acid-D-Ala-D-Ala, was probably formed by an N-acetylmuramyl-L-alanine amidase active on the peptide side chains of The uncross-linked polymer. The uncross-linked peptidoglycan polymer was shown to be a good substrate for penicillin-sensitive D-alanine carboxypeptidases purified from membranes of B. subtilis, Bacillus stearothermophilus, and Escherichia coli. D-alanine release was not, however, coupled to the cross-linking of peptide side chains, suggesting that these enzymes do not function as peptidoglycan transpeptidases in vivo. No transpeptidase or D-alanine carboxypeptidase activity was detected in mixtures of high molecular weight penicillin-binding proteins from B. subtilis, B. stearothermophilus, or Staphylococcus aureus. Possible reasons for the inability to demonstrate these activities are discussed. In addition, an N-acetylmuramyl-L-alanine amidase activity which copurifies with penicillin-binding proteins from B. subtilis, S. aureus, and E. coli was partially characterized.

Time-resolved fluorescence spectroscopy of spinach chloroplast

Picosecond fluorescent kinetics and time-resolved spectra of spinach chloroplast were measured at room temperature and low temperatures. The measurement is conducted with 530 nm excitation at an average intensity of 2-10(14) photons/cm2, pluse and at a pulse separation of 6 ns for the 100 pulses used. The 685 nm fluorescent kinetics was found to decay with two components, a fast component with a 56 ps lifetime, and a slow component with a 220 ps lifetime. The 730 nm fluorescent kinetics at room temperature is a single exponential decay with a 100 ps lifetime. The 730 nm fluorescence lifetime was found to increase by a factor of 6 when the temperature was lowered from room temperature to 90 K, while the 685 and 695 nm fluorescent kinetics were unchanged. The time-resolved spectra data obtained within 10 ps after excitation is consistent with the kinetic data reported here. A two-level fluorescence scheme is proposed to explain the kinetics. The effect of excitation with high light intensity and multiple pulses is discussed.

Fluorescent kinetics of chlorophyll in photosystems I and II enriched fractions of spinach

The fluorescent emission kinetics of spinach subchloroplast Photosystems I and II particles have been studied on a picosecond time scale. Using picosecond laser pulses and an optical Kerr gate, the fluorescent decay times are measured to be 60 plus or minus 10 ps, and 200 plus or minus 20 ps for Photosystems I and II, respectively. The quantum yields are calculated to be 0.004 for Photosystem I and 0.013 for Photosystem II. Theory of exciton energy transfer and trapping is applied for the determination of intermolecular potential energyin the photosystems.