Exact(11)
Line 9 adds the estimated C j to C. When the loop terminates, C contains throughput capacities, C j, for each user j∈S.
We observe in Figure 3 that the ergodic capacities C erg FR1 ( H pl, 0 ) and C erg FR3 ( H pl, 0 ) intersect for values of the shadowing standard deviation up to 6 dB.
These maximal BSS capacities c kz are calculated for the cases of guaranteed voice/data rate combinations equal to 12.2/384, 12.2/128, and 12.2/64 kb/s.
Multipliers λ i (t) and capacities c i (t) do not converge, but ergodic rates c ̄ i ( t ) do. Figure 4 Optimal frequency division broadcast channel.
The Einstein temperatures extracted from the volume versus temperature data are in reasonable agreement with values determined from heat capacities (C v) simulated as a function of temperature using the results of the DFT phonon calculations (121 and 801 K).
First, we see that both ergodic capacities C erg FR1 ( H pl, 0 ) and C erg FR3 ( H pl, 0 ) are constant for high path losses (i.e., close to the AP).
Similar(49)
Considering Gaussian distribution for the channel capacity (C k ), the close-form expression for outage capacity, i.e., C q k can be derived.
The total heat capacity C for n moles is defined by C = nc.
From κ and λ, heat capacity, C, was also derived.
The total heat capacity C for n moles is defined by C = nc.
The sorption capacity (C) is an absolute criterion to characterize the efficiency of the CO2 capture.
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