Plant organs such as leaves or petals move as a result of changes in the shape and/or the volume of motor cells. In a similar manner, stomates open and close when the turgor in the guard cells changes. The time scale of such movements ranges from several milliseconds to hours. The most detailed studies of cellular movement have been done with stomata. Stomatal opening requires the uptake of K+ by guard cell, and the presence of K+ channels in their plasma membranes and tonoplasts that mediate this K+ flux (Fischer, 1968). If water follows K+ flux by osmosis, then the rate of flux would determine the rate of volume change (Schroeder et al., 1984). This explanation is frequently used as a paradigm for other nyctinastic and seismonastic movements (Moran et al., 1990; Fleurat-Lessard et al., 1997; Moshelion and Moran, 2000). For example, in Mimosa pudica, the observed potassium exchanges and the nature of the anatomical structures of pulvinule and pulvinus have led to suggestions that movements are the result of modifications in the volume of motor cells at the base of each leaflet and leaf by a “lever” effect. However, none of the movements in plants is really understood at the molecular level. Here, we discuss the constraints brought to the paradigm of movement by considering the values of cell membrane transport parameters and the characteristic time of the movement.
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Morillón et al. (2001) studied this question.
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