The second, or power, component of the current is in phase with the voltage applied to the stator, while the first, or magnetizing, component lags the applied voltage by a quarter cycle, or 90°.
For this paper, a positive-first biphasic voltage pulse, applied to one electrode at a time, was used in all experiments.
To evaluate coupling conductance, 20-mV pulses for 7 seconds were applied to one cell to establish a transjunctional voltage gradient (Vj), while the junctional currents (Ij) were measured in the other cell.
An asymmetrical square wave voltage is applied to one electrode.
The total sweeping distance (L) between the first and the last spots increased linearly with the voltage applied to the galvo mirror, exhibiting the slope of 0.25 pixel/mV (Supplementary Fig. 3b).
Thus, if the gates of an n-type and a p-type FET are connected any voltage applied to the common gate will operate the complementary pair, turning one on and leaving the other off.
We then measure the light intensity transmitted through the second PBS as we vary the voltage applied to the LC.
The amount of current that flows between the source and drain is determined by the voltage applied to the gate.
To avoid this occurrence, a compensation voltage (CV) is applied to one electrode.
To determine a touch coordinate, power is applied to one sheet and voltage is read off the other, the location of the touch will result in larger or smaller division of the voltage divider and result in varying output voltages.
To flip the switch, a small voltage is applied to a third superconducting layer.
