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The strip, connected to the negative side of a direct current through large-diameter conductor rolls located above and between two cells, is dipped into a tank of electrolyte by a submerged sink roll.
Discharge across the boundary between two cells is calculated if the ground height in the dry cell is lower than the water level in the submerged cell; otherwise, the discharge is considered to be zero (Imamura, 1996).
Using a computational model it is shown that the pattern of intra-hemispherical connections can be accounted for by assuming that the connection probability between two cells is dependent primarily on two factors — receptive field overlap and orientation selectivity.
The horizontal handoff rate between two cells is λ wc c → c, whereas the vertical handoff rates from a WLAN to a cellular network (upward vertical handoff) and from a cellular network to a WLAN (downward vertical handoff) are denoted by λ wc w → c, and λ wc c → w, respectively.
A linkage between two cells is the edge of the network, denoting the interaction strength between cells.
For example with the cellular Potts model, the number of lattice boundaries shared between two cells is counted and included as a term in the model's energy function.
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The differences in spot intensities between two cells were analyzed in Fig. 3a.
The maximum difference between two cells was found at 43 mV.
Using live imaging, we show for the first time that transient contacts between two cells are sufficient to transfer OM materials, proteins and lipids, at high efficiency.
Ducret et al. observed that contact between two cells was sufficient to stimulate transfer of proteins and lipids from the outer membrane.
The number of links between two cells was set as k = 4, and the initial population of type A and type C cells were set as 9900 and 100, respectively.
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