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Analytical precision (i.e., coefficients of variation for triplicate measurements) was within 3%% for Na+, NH4 +, K+, Mg2+, Ca2+, F−, Cl−, Br−, SO4 2−, Fe, Mn, Si, and Sr; 4 % for P; and within 11%% for NO3 −.
This part compromises the energy consumed by the K SR hops to reach the last relay, which can be written as follows E s t 2 = K P T x S R + P R x S R + N + 1 - 1 / K P SlSR N L / R SR (4).
Sr isotope ratios in solids and fluids are identical under equilibrium conditions, so the Sr isotope ratio in the solid after interaction with the fluid, (87Sr/86Sr s, is given by S 87 r / S 86 r s = S 87 r / S 86 r s 0 ⋅ C s 0 Sr C s 0 Sr + R ⋅ C f 0 Sr + S 87 r / S 86 r f 0 ⋅ R ⋅ C f 0 Sr C s 0 Sr + R ⋅ C f 0 Sr (4).
Two miles later, a concurrency begins with SR 4.
One mile later, the concurrency ends with SR 4 continuing to move north.
Oregon Way continues after the end of SR 433 into downtown Longview and SR 4.
Similar(19)
The shifts are estimated from the LR frames the same way they are for SR [4].
The following values are considered and fixed throughout this section in which most of them are also used in [6]: T f =105 μs, T sr =4 μs, β (i =0.9 and W (i =5 MHz, for all i.
The corresponding strain can be drawn using Equation (6) as ϵ sm = ϵ cr + ϵ s - ϵ sr 2 + 1 2 ϵ s - ϵ sr ϵ s + 3 ϵ sr - 4 ϵ cr, Open image in new window (7).
For example, with the simulation parameters, d sr ≈4 m is the optimal distance to achieve the best secrecy rate for the optimal scheme, w J ⊥h jd scheme, w J ∥h je scheme, w R ⊥h re scheme, and CB scheme.
In Fig. 5, the consistency of the lower-bound analyses for both the fixed-gain and variable-gain AF-FD relaying are demonstrated where the system parameters are chosen as 2P S =3P R, Ω SR =1, Ω RD =2, Ω LI =0.025, m SR =4, m RD =2.5, m LI =1 and γ th =4.
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