* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download experiment 1
Electric power system wikipedia , lookup
Nominal impedance wikipedia , lookup
Stray voltage wikipedia , lookup
Wireless power transfer wikipedia , lookup
Audio power wikipedia , lookup
Scattering parameters wikipedia , lookup
Current source wikipedia , lookup
Power inverter wikipedia , lookup
Electrification wikipedia , lookup
Pulse-width modulation wikipedia , lookup
Voltage optimisation wikipedia , lookup
Mains electricity wikipedia , lookup
Electrical grid wikipedia , lookup
Variable-frequency drive wikipedia , lookup
Opto-isolator wikipedia , lookup
Electrical substation wikipedia , lookup
Switched-mode power supply wikipedia , lookup
Power electronics wikipedia , lookup
Buck converter wikipedia , lookup
Electric power transmission wikipedia , lookup
Three-phase electric power wikipedia , lookup
Amtrak's 25 Hz traction power system wikipedia , lookup
Power engineering wikipedia , lookup
Alternating current wikipedia , lookup
Transmission line loudspeaker wikipedia , lookup
INTERPRETATION OF RESULTS Part I. TRANSMISSION LINE DEMONSTRATION A. Propagation in a Transmission Line - The output voltage is generally set to zero and switched for ‘step input to A,’ (source-toload) there’s a two units amplitude and propagating it reversibly (‘step input to B’) the pulse propagates from the load to the source. - We raised the output voltage of the generator, we observed that the amplitude gradually increases and decreases while there’s a constant amplitude when we haven’t raised the output voltage. - We computed for the wavelength, λ, using the formula λ = v/f wherein the v = 4L and the f = 0.25s and we computed the wavelength 16L for the given line. B. Attenuation and Dispersion - We set the attenuation control to ‘min’ but when we gradually raise it to ‘max’ there’s a sudden delay in the transmission line or in other words the amplitude decreases as signals approaches to the load (preferably delay in filling amplitude units). - The attenuation decreases as we reduce the frequency of the generator, some of the causes of attenuation are the resistance and skin effect; conductance and dielectric losses. - The amplitude decreases as it approaches the load because there’s no generator to supply the frequency on transmission. - We observed a reflected wave because we transfer the 600R terminator from ‘B’ to ‘A’ end of the line and operate the ‘step input to B’ switch. C. Terminations, Simple Cases (matched line, open circuit, short circuit) - When the transmission line is properly terminated, the transmitted pulse propagates from source and the maximum power will be transferred to the load, there is no reflected wave. - If the line is not properly terminated, some of the energy will enter the load and some will be reflected back toward the source. The greater the mismatch between the load and the line, the greater are the reflections on the line. - Some of the energy traveling back toward the source will cancel the forward energy or some will add to the forward energy. - The standing wave at the termination B is in maxima (antinode) when the function generator output raised to give a traveling wave of about half-scale amplitude. - The short-circuit link is in parallel with the termination ‘B’, the standing wave is minimum because of the 180o phase reversal of the incident and the reflected wave, thus canceling out. Part II. STANDING WAVE AND PARTIAL REFLECTION - Our observation on the reflected pulse, the value of our reflection coefficient in 1kOhms is equal to 0.5 and in 200R is -0.5. It also agree with the calculated value Z b Z o / Z b Z o . - Maximum amplitude will occur in terms of the reflection coefficient when the reflected and incident waves sum up. Add to this, if the reflection coefficient is high, the maximum voltage is also high and maximum amplitude also occurs. - As we properly terminated the source and the load, we observed a phase shift in the minimum and maximum points, because one of the output is 180o out of phase. CONCLUSIONS - The proper use of a transmission line is to terminate it in a load impedance equal to its surge impedance. All the power applied to the line will be absorbed by the load. - Wavelength is the distance between adjacent peaks of an RF wave. It is also the distance traveled by a signal in one cycle. - The characteristics of the transmission line are determined by the length of the line, the size of the wires and the dielectric material used between the wires. - If a transmission line is not terminated in its characteristic impedance, the load will not absorb all the power, some of it will be reflected back to the generator. - If the load on the transmission line is open or short, all the power applied to the line will be reflected back to the generator. - The forward or incident power applied to the line combines with the reflected power to produce a pattern of voltage and current variations along the line known as standing waves. - If the load impedance matches the line impedance, there are no standing waves. - A measure of the mismatch between line and the load impedances or the maximum and minimum voltage and current variations along the line is the standing wave ratio (SWR) which is a number always greater than 1. - In a balanced transmission line, the energy in each wire or line is 180o out-of-phase with the opposite line and hence the fields of the two lines cancel. -In an unbalanced transmission line, one line is at ground potential while the other line conducts RF energy. - The SWR indicates how much power is delivered to the load and lost in the line. With SWR =1, all power is delivered to the load.