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For cell membranes, the intracellular liquid is usually denoted as solution 2, while solution 1 is the extracellular liquid. The formation of a membrane potential is connected with the presence of an electrical double layer at the surface of the membrane. For a thick, compact membrane, an electrical double layer is formed at both interfaces. The electrical double layer at a porous membrane is formed primarily in the membrane pores (see Section 6.2). The electrical double layer at thin membranes is formed on both membrane surfaces. It is formed by fixed ions on the surface of the membrane and the diffuse layer in the electrolyte. Consider the simple case where both sides of the membrane are in contact with a solution of symmetrical electrolyte BA in a single solvent and the membrane is permeable for only one ionic species. In equilibrium its electrochemical potential (Eq. (3.1.5)) in both solutions adjacent to the membrane has the same value. Thus,



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In view of this equation the effect of the ionic atmosphere on the potential of the central ion is equivalent to the effect of a charge of the same magnitude (that is zke) distributed over the surface of a sphere with a radius of a + L D around the central ion. In very dilute solutions, LD a; in more concentrated solutions, the Debye length L D is comparable to or even smaller than a. The radius of the ionic atmosphere calculated from the centre of the central ion is then L D + a. Work w2 can now be calculated and, from this value, the total electric work Wel, found in an analogous way to that previously used for the case of the limiting law, yielding Ve2 Y Nz2 ln W*i= - A (! + K ) 3 V t





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If the number of available links is less than or equal to the threshold value, the LAG is declared operationally down until the number of available links is greater than the threshold value.

The side panels of the G11 also include: Speaker. A speaker is included on the left-hand side of the G11 to listen to audio after recording movies. DC coupler cable cover. When using the optional AC Adapter Kit ACK-DC50, the coupler cable that connects the camera to household power exits the camera via this opening on the right side that is closed by the cover when the camera uses a standard NB-7L battery.

+ 2(*a)]

When the number of available links is less than or equal to the threshold value, dynamic costing is used to determine the advertised LAG cost.

(L3.28)

Listing 4.1 illustrates an example of configuring a LAG group with the port-threshold option of down.

(The expression in square brackets follows from the integral a3 J [q2/(l + Ka)] dq after introducing the limits 0 and zke.) The expression for the activity coefficient is calculated from the differential dWjdnk (neglecting the dependence of V on nk) by substitution into Eq. (1.3.21). Rearrangement yields

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Config> lag Config>lag# Config>lag# Config>lag# Config>lag# Config>lag#

/2P2N () \

1 description LAG from PE1 to PE2 port 2/1/1 2/2/1 3/1/1 port-threshold 2 action down dynamic-cost no shutdown

A big part of the excitement of the new G11 is the new high-resolution 2.8-inch variangle PureColor II VA LCD. Although slightly smaller than the 3.0 inch LCD monitor on the previous G10, it includes the same number of pixels, and the smaller size allows the LCD to be positioned for shooting comfort and functionality, or completely ipped around to protect the face of the LCD when the camera is not in use. You use the LCD to compose images while shooting, review images and videos during Playback mode, and operate the menus. As an added feature, the LCD monitor brightness level can be set over a ve-step range, convenient when shooting in brightly lit situations or when shooting in low-light locations where the glow of the LCD may be distracting to others.

The numerical value of this constant is B = 1.5903 x 10 10 (D7r 1/2 = 502.90(DTym m1/2 mol"1/2 dm3/2 mol" m nm"1

As illustrated in Listing 4.1, dynamic cost can actually be configured as a general command and not just as a port-threshold option. If dynamic cost is enabled, then it affects the OSPF routing protocol cost (we discuss the OSPF routing protocol and

and, for water at 25 C, B = 1.0392 xl0 8 m 1 / 2 -mor 1 / 2 = 3.2864 dm3/2 m o P m nm"1 In the above two equations, the former value is valid for basic SI units and the latter value for / in moles per cubic decimetre and a in nanometres. The parameter a represents one of the difficulties connected with the Debye-Hiickel approach as its direct determination is not possible and is, in most cases, found as an adjustable parameter for the best fit of experimental data in the Eq. (1.3.29). For common ions the values of effective ion radii vary from 0.3 to 0.5. Analogous to the limiting law, the mean activity coefficient can be expressed by the equation

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