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Moreover, its combustion efficiency is stable in a wider combustion load (input power) range.
It can be seen that, from the constellation diagrams, L4 generates higher IMD than L0 does within low input power range, while L0 generates higher IMD than L4 does within high input power range.
For the whole input power range, the heat transfer coefficients have almost the same trends for boiling silver-water nanofluids and water.
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Avionics thermal behavior was simulated by employing electrical resistances with input power ranging from 40 to 850 W.
The performance of the circuits was measured in terms of the power conversion efficiency (PCE), and this characterization was done for RF input power ranging from 20 dBm to 0 dBm.
Accordingly, for an input power ranging from 120 to 240 W, the enhancement of the average heat transfer coefficient for nanofluids relative to pure water is about 30%to38%8% for 25 mg/L and 56%to77%7% for 50 mg/L silver concentrations, respectively.
It can be seen that L0 generates the lowest spectra regrowth than others do within low-input power range, while it generates the highest spectra regrowth within high-input power range.
The performance of different predistorter model are analyzed for input laser power ranging from −4dBm to 4dBm, input frequency for ∼0.55 GHz to ∼3.00 GHz and for different type of input signal like m-QAM, orthogonal frequency division multiplex, WiMax and LTE (long term evolution).
A plot of the required input power over the range of operation can be found in Figure 2.
We have also studied the power dependence of the attenuation constant which we find to be independent of the input power in a range from −140 to (-80 mbox{dBm}) (see Appendix 5).
We find the measured attenuation constant of CC085NbTi to be independent of the input power in a range from −140 to (-80 mbox{dBm}) corresponding to an average photon number on resonance inside the resonator of 105 to 0.2 and an average resonator voltage (langle V^{2} rangle^{1/2}) of approximately 10−6 to (10^{-4} mbox{V}) (Figure 9).
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