Different weights for the mechanical and electrical contribution to switching are selected phenomenologically to simulate electric displacement vs electric field and strain vs electric field of a ceramic lead lanthanum zirconate titanate (PLZT).
The values of V and AF along all the 12 lines have been calculated for the three considered stimulation conditions: macroelectrode, microelectrode in position 1 and microelectrode in position 2. In Figure 5, the electric potential V is reported along the 3rd line), belonging to the group L1 7, and the 11th line), belonging to the group L8 12, for the three kinds of stimulation.
Surface atoms are evaporated by means of electric pulses V p added to the DC voltage V 0 and are collected on a position sensitive detector.
Now looking for energy stats re cooking in electric oven v cooking on gas hob.
Interpretation of numerical values like electric voltage (V), Mechanical displacement and Vonmises stress.
The corresponding J-V characteristics are plotted in Figure 8c,d, based on the previously calculated Jsc and the dark current densities under continuously increasing forward electric bias (V).
We conclude the main result in the following: Assume that (H1) holds and the electric potential V is a continuous differentiable function.
For low electric potential ((v = 0.054)), the low energy bands show a Mexican hat shape with a gap energy of 0.054 as observed experimentally [8, 23].
We consider a two-dimensional massless Dirac operator coupled to a magnetic field B and an electric potential V growing at infinity.
It is expressed by the criterion (varvec{E} + varvec{V} times varvec{B} = 0), where E is the electric field, V is the plasma bulk velocity, and B is the magnetic field.
The electric potential V exhibits the same behavior for all the fibers of group L8 12.
