From the figure, it can be seen that, for example, for data rate Rb = 103 bits/s, an operating range larger than 20 m can be achieved.
It can easily be seen that, in this example, the best lower bound is the first one given by Theorem 3.5.
It can be seen that for this example, the most important impulsive effects are the first two impulsive functions b 1 and b 2. In this paper, we first put forward a model of second-order impulsive differential systems with Erlang distribution random impulses.
In addition, it can be seen that in small examples, both SA and TS find a global optimum.
It can be seen that in these examples, different positive externality "drivers" lead to equivalent (threshold) micro-scale models.
Finally, from Figures 1-8, it can be seen that the numerical solutions of Example 2 are less ideal than these of Example 1.
The purple curve was developed using a standard generic curve fitting model, and it may be seen that the capacity for this example is 2,110 veh/h/ln.
As an example, it is seen that the PL peak position of the GaAs/GaInAs MQW shell with a thickness of 8.5 nm is very close to that of a planar 8-nm-thick GaAs/GaInAs MQWs.
The main advantage of shortening the loop according to Section 3.2 can be seen in that, for example, in continuous operation, it is not necessary to perform the last iteration and it is possible to start processing the input sample x[N] in the time spared.
It can be seen, for example, that for a relatively small flat (studio or 1-bedroom), a transmission power of −4 dBm would be able to provide sufficient in-house coverage, whilst requiring 33%% less energy for BLE packet transmissions.
