Simplified Method for Isolation and Separation of Bacterial Nanowires from Pseudomonas aeruginosa

2015 ◽  
Vol 2 (1) ◽  
pp. 43-48 ◽  
Author(s):  
Muthusamy Anand ◽  
Muthusamy Maruthupandy ◽  
Akbar Sait Hameedha Beevi ◽  
Radhakrishnan Jeeva Priya
1973 ◽  
Vol 26 (1) ◽  
pp. 120-121
Author(s):  
Lois F. Jones ◽  
B. V. Pinto ◽  
Evan T. Thomas ◽  
J. J. Farmer

2020 ◽  
Author(s):  
luyan ma

<p>Microbial nanowires are nanofilaments that could offer an extracellular electron transfer (EET) pathway linking the bacterial respiratory chain to external surfaces, such as oxidized metals in the environment and engineered electrodes in renewable energy devices. Filaments proposed to function as nanowires have been reported in multiple bacteria, yet it remains largely unclear about the composition and electron transfer mechanism of bacterial nanowires. Pseudomonas aeruginosa is an environmental and electrochemically active bacterium. In this study, we found nanotube-like extracellular filaments in P. aeruginosa biofilms, which were bacterial membrane extensions similar to the nanowires reported in Shewanella oneidensis. Remarkably, conductive probe atomic force microscope showed measurable conductivity of these extracellular filaments, suggesting that they may function as nanowires in P. aeruginosa. Our results also indicated that the electron shuttle pyocyanin significantly affected the conductivity of P. aeruginosa nanowires, suggesting that the electron transfer mechanism of P. aeruginosa nanowires was different from S. oneidensis. Furthermore, factors that impact biofilm formation, such as flagella, type IV pili, and exopolysaccharides, were not essential for nanowires formation, while affect the formation and length of nanowires of P. aeruginosa. Taken together, this is the first report that investigated the role of electron shuttle on the conductivity of nanowires and factors that affected nanowires formation.</p>


Author(s):  
Muthusamy Maruthupandy ◽  
Muthusamy Anand ◽  
Govindhan Maduraiveeran ◽  
Akbar Sait Hameedha Beevi ◽  
Radhakrishnan Jeeva Priya

1973 ◽  
Vol 26 (1) ◽  
pp. 120-121 ◽  
Author(s):  
Lois F. Jones ◽  
B. V. Pinto ◽  
Evan T. Thomas ◽  
J. J. Farmer

1974 ◽  
Vol 27 (2) ◽  
pp. 400-406 ◽  
Author(s):  
Lois Faye Jones ◽  
J. P. Zakanycz ◽  
Evan T. Thomas ◽  
J. J. Farmer

1974 ◽  
Vol 27 (2) ◽  
pp. 400-406
Author(s):  
Lois Faye Jones ◽  
J. P. Zakanycz ◽  
Evan T. Thomas ◽  
J. J. Farmer

Author(s):  
K. Yoshida ◽  
F. Murata ◽  
S. Ohno ◽  
T. Nagata

IntroductionSeveral methods of mounting emulsion for radioautography at the electron microscopic level have been reported. From the viewpoint of quantitative radioautography, however, there are many critical problems in the procedure to produce radioautographs. For example, it is necessary to apply and develop emulsions in several experimental groups under an identical condition. Moreover, it is necessary to treat a lot of grids at the same time in the dark room for statistical analysis. Since the complicated process and technical difficulties in these procedures are inadequate to conduct a quantitative analysis of many radioautographs at once, many factors may bring about unexpected results. In order to improve these complicated procedures, a simplified dropping method for mass production of radioautographs under an identical condition was previously reported. However, this procedure was not completely satisfactory from the viewpoint of emulsion homogeneity. This paper reports another improved procedure employing wire loops.


Author(s):  
Yeshayahu Talmon

To bring out details in the fractured surface of a frozen sample in the freeze fracture/freeze-etch technique,the sample or part of it is warmed to enhance water sublimation.One way to do this is to raise the temperature of the entire sample to about -100°C to -90°C. In this case sublimation rates can be calculated by using plots such as Fig.1 (Talmon and Thomas),or by simplified formulae such as that given by Menold and Liittge. To achieve higher rates of sublimation without heating the entire sample a radiative heater can be used (Echlin et al.). In the present paper a simplified method for the calculation of the rates of sublimation under a constant heat flux F [W/m2] at the surface of the sample from a heater placed directly above the sample is described.


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