Noise is a pervasive feature of many microbial processes. Cells moving in a real
environment, as contrasted with controlled laboratory conditions, experience more
than one source of noise, some present within the cells (Rao et al., 2002), some
emanating from the extracellular environment (Patnaik, 2006a), that is, the noise
associated with the binding process between the cells and chemicals from the
environment.
The third source of noise is significant in the chemotaxis of bacterial and other
cells. This study concentrates on bacterial chemotaxis not because the chemotaxis of
other types of cells is unaffected by binding noise, but because their mechanisms
and responses are different (Levchenko and Iglesias, 2002; and Andrews et al., 2006).
Studies of bacterial chemotaxis have generally employed Escherichia coli
(E. coli) as a model system because of its well-understood biochemistry, the simplicity
of its chemosensory network and its usefulness as a host for genes from other cells.
Chemotaxis refers to the movement of cells in response to chemical stimuli.
If the stimulus is favorable, the cells move toward it; similarly, they move away
from unpleasant or hostile stimuli. The former phenomenon is chemoattraction,
and it forms a major fraction of useful chemotactic processes. To decide their
directions of movement, bacteria should sense the gradient of a chemoattractant.
This is done by comparing the concentration of the chemoattractant at two points,
either on the cell surface, or across a span of time. Since E. coli are small, spatial
differences across a cell are not significant. The cells therefore determine a favorable
direction by comparing the chemoattractant concentration as they move along
(Baker et al., 2006).
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