CHAPTER 6
RESULTS & DISCUSSION
The antenna configuration shown in the last chapter are now being represented in their respective output form. In order to represent it we would be displaying the plots like Return Loss, VSWR plot, Impedance plot, Electric field radiation plot and smith plot. The basic objective behind showing these plots is to justify that the designed antenna will radiate efficiently.
6.1 Results: Antenna Configuration 1:
6.1.1.Return Loss Plot: Return loss is a measure of how well devices or lines are matched. A match is good if the return loss is high. A high return loss is desirable and results in a lower insertion loss. Fig. 6.1.1 Return Loss Plot for Antenna Configuration 1
6.1.2 VSWR Plot: VSWR is the voltage ratio
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It can also be derived from the impedances:
VSWR = (1+ )/(1- )
Fig. 6.1.2 VSWR Plot for Antenna Configuration 1
6.1.3 Smith Plot: The scattering matrix is a mathematical construct that quantifies how RF energy propagates through a multi-port network. The S-matrix is what allows us to accurately describe the properties of incredibly complicated networks as simple "black boxes". For an RF signal incident on one port. The same is being shown here in the manner of Smith Plot. Fig. 6.1.3 Smith Chart Plot for Antenna Configuration 1
6.1.4 3D Rectangular Plot: The plot well describes the representation for all curves having return loss less than -10dB. Fig. 6.1.4 3D Rectangular Plot for Antenna Configuration
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6.4.1 Return Loss Plot for Antenna Configuration 4
6.4.2 Smith Chart: The incident voltage at each port is denoted by "a", while the voltage leaving a port is denoted by "b". Don't get all hung up on how two voltages can occur at the same node, think of them as traveling in opposite directions!
Fig. 6.4.2 Smith Chart Plot for Antenna Configuration 4
6.4.3 3D Rectangular Plot: The current plot is of the sense that at the observed solution frequency we are getting a consistent growth for return loss. The double dips in the plots are showing that we are getting 2 curves with return loss is below -10dB Fig. 6.4.3 3D Rectangular Plot for Antenna Configuration 4
6.4.4 Impedance Plot:
Fig. 6.4.4 Impedance Plot for Antenna Configuration 4
6.5 Antenna Configuration 5:
6.5.1 Return Loss Plot: The most efficient plot of all the designed configurations in which a return loss of around -40dB is obtained with a significant growth in Bandwidth as
Measure the capacitance of the coaxial cable(*10 probe) 2. Determine Ra and Rb to meet the amplitude and Tau. 3. Connect the circuit as shown in Fig. 2 4. Switch the oscilloscope to 50 kHz square wave, 11 peak-to-peak voltage.
In half-duplex networks, the node transmitting must make sure that the network is quiet prior to transmitting, and in addition there is usually some mechanism for transmitting nodes to detect overlapping transmissions. 10BASE5 coaxial cable is the transmission technology used in the classic Ethernet protocol which was a stiff enough cable which was hard to install in buildings etc. as it was hard to bend. As it was hard to install along with other issues, 10BASE2 cable was made which was a skinnier coaxial cable which had obvious improvements in terms of installation.
For this experiment we utilized varying forms of Ohm’s law (V=IR), rules for resistors in series (Rtotal=R1+R2+…) and parallels (1/Rt=1/R1+1/R2+⋯), and Kirchhoff’s Junction Rule (ΣIi=0). For these models we assumed that the DMM’s produced accurate readings
The energy associated with each node would be displayed with each node. The nodes except the main source (that are fixed) are mobile. Energy Calculation: …………………………………………………………….Equation 9.2 Where, B= Magnetic flux density(Magnetic flux density is defined as the amount of magnetic flux in an area taken perpendicular to the magnetic flux 's direction.)
section{Evaluation} label{sec-analyze} vspace{-0.08in} We evaluate Tarax with the six popular server applications described above. We first perform experiments to compare the performance and code sizes of the Tarax-optimized kernels and the vanilla kernel. We then perform dynamic profiling on the kernels to collect detailed statistics on instruction cache misses and branches. Finally, we switch on specific GCC optimizations with and without profile feedback, respectively, to collect performance numbers.
Once, the current rating and voltage rating are chosen, one needs to look at the data sheet of the connector to check whether it meets the given specifications. In the datasheet, one should look at the test procedure used to arrive at the specifications and check whether it meets the test standard. Not everyone uses the same testing criteria, so ensure you understand how these specifications were derived. It should also be confirmed that the contact will support the conductor size that has been chosen. A non-compatible conductor could cause overheating issues, leading to premature connector failure.
We model the time-variations of each of the channels by a first-order Gaussian autoregressive process whose parameters are selected in such a way that their autocorrelation values match to the autocorrelation of the fading process of their corresponding channels. The fourth channel model,
In Figs. (\ref{fig:NC3Mont.eps}-\ref{fig:NC6Mont.eps}), the results of the Monte Carlo analysis is presented along with the result obtained for the central values of the parameter. It is observed that for the form factors $C_3^{N \Delta}(Q^2)$, $C_4^{N \Delta}(Q^2)$ and $C_6^{N \Delta}(Q^2)$, Monte Carlo analysis and the prediction for the central values agree at large values of $Q^2$, but deviate from each other for small values of
The numbers $N_{\omega}^{rec}$ and $N_{\omega\to\pi^0\gamma}^{rec}$, extracted from the different combinations for two energies, are plotted in Fig.~\ref{fitbr15sysin} and Fig.~\ref{fitbr15sysex}, respectively. The numbers are listed in Appendix~\ref{fitsysematicinclusve} for reference. The distributions are fitted with a constant fit to have the error estimate.
If the two stations begin the transmission at the same time the signal will interface after exactly 250m. Tinterface = 375m 200 x 106 m/sec. = 1.875 μsec T(bit - times) = 107 x 10-6 x 1.875
However, this would be difficult since it would be hard to determine the size of the connected component and it would be easy for the components to get connected together through one edge. Therefore, I went into the experiment with the mindset that I should connect to the immune vertex in the biggest component. 2. My strategy employed during the
For Herbert Run the conductivity level was 687µS/cm. The Turbidity level was 0 FAU and the Nitrate level was 0.02ppm. I accept my hypothesis and reject parts of my hypothesis. I reject that both streams have a high turbidity level. Both streams’ turbidity level is zero.
1.) The life of slaves in the 1700 could be easy, or hard, depending on their “master.” Some slaves worked on farms and performed extremely hard feats of work, but others would do house work for their master that was not as hard but more time consuming. Now these slaves were like servants, but they are considered property, unlike a servant that is a free person. Since slaves were considered property their master could do anything they to them, like branding them just for not doing as told.
Oaks Mall in Gainesville, Florida, which is in northern Florida. The largest city in Alachua County, Gainesville is the largest growing populated city in Florida. Oaks Mall 's anchor stores include Belk, Sears, JCPenney, and Macy 's, and opened in 1978. Whether you 're done getting all that fun shopping done, or you just want to head to a nearby restaurant, you can hop over to Crafty Bastards Restaurant and Pub! Sometimes the old adage "when in Rome" is just so applicable.
[3] This pattern is also linked to Equations 1&2 as stated previously. The position of every fourth fringe was recorded giving the value which is required in Equation 3 below. (See Table1 for the recorded data) Knowing the wavelength of sodium to be 589nm the angle, ,at the apex between the two glass plates can be calculated using Equation 3 as