The potential T at a point P can be expressed in terms of anomalies Δ g(Q) at points Q on an exterior boundary σas 1where R is the reference radius of the surface (1738 km in our case) and the kernel S P, Q) is the Stokes-Pizetti kernel [ Heiskanen and Moritz, 1984].
The potential at a given point is the sum of the Coulombic contribution from both discrete source and continuous induced charges.
We define "reaction potential" the electrostatic potential at a given point due to induced charges only: Φ R ( r ) = 1 4 π ε 0 ∑ i = 1 N h i a i r - r i (5).
Let the y and z dimensions of the array be L × L. The vector potential at a far point due to the current distributions is A → r →, t = μ 0 4 π ∫ J → 2 Ω r → ', t − R / c / R ) dV ' + ∫ J → 2 Ω ' r → ', t − R / c / R ) dV ', Open image in new window (15).
The electric potential at any point is defined as the energy required to bring a unit test charge from an infinite distance slowly to that point.
According to the initial work of de Lorente (56), the potential at an observation point [z 0, y 0] can be expressed by equation 18: where z and y are the axial and radial directions, respectively, S1 and S2 are the fiber sections at the fiber ends and r is the distance between the surface elements dS and the observation point.
While everyone else has been defining Strawberry's potential, he remains at a point when he still has to define himself.
In a similar manner, Bagherbandi (2011) modified Eq. (1) to recover the second-order radial derivative of the compensation potential instead of the compensation attraction: (2) where is the second-order radial derivative of the disturbing potential T * (P) at a point P and stands for its topographic effect (see e.g. Wild and Heck, 2004a, b; Eshagh and Sjöberg, 2008; Bagherbandi, 2011, chap. 4).
Experiments for generating osmolarity plots were performed at an inward positive membrane potential at an incubation time point of 10 min (see section 2.5.1.1).
ted wrote: If two or more neurites are connected at a common point, the potential at that point is calculated algebraically as the weighted sum of the potentials of the adjacent internal nodes, where the weights are the reciprocals of the axial resistances between the common node and the adjacent internal nodes.
