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Transmission Line - Science topic

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in transmission line differential protection this a big issue
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Misalignment mainly occurs due to differences in phase angle and ratio error of CTs used, as are cannot be identical but with proper compensation the error of leakage current could be minimized……
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Hi,
I get confused about the CST calculations for reflection and transmission values (S- S-Parameters) for different kinds of transmission lines.
1)First could you please let me know where is the evanescent port mode selection available in CST for waveguide port?
2)If I want to see the S11 parameters of a rectangular waveguide, how does the CST calculate it?
Explain more:
The input impedance of a rectangular waveguide is its wave impedance of dominate mode. So the Zte impedance is not fixed and it varies with frequency. (attachment formula)
So, what type of and what value of waveguide port impedance is considered, for calculating the S11 parameters during the total bandwidth of a dominant mode and also more than dominant mode bandwidth?
3) If the type of TLs are not common or some changes are made, how does CST calculate the S11 for these structures? For popular TLs such as waveguides, we have a common formula.
I appreciate your time and explanation in advance.
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I wouldn't expect CST to be that accurate for S21. If you don't run it for very long you have power still bouncing around inside the problem, and if you run it for a long time then numerical errors start to build up. How much ripple was there left on the S11? If you watch the S11 as the solution progresses you can see the ripple reduce every time a lump of energy arrives at the port (see the energy monitor). If the finishing point is -40 dB energy left there is still 0.01% of the energy left in the problem which has the potential to make +/-1% difference in the voltage at the output port which is */-2% of the power. The absence of this from the answer leaves ripple in the S parameter. This ripple is bigger than the differences you are seeing. I'm not sure that the impedance is calculated as you would hope, but I think you can't tell from these results if it's right or not.
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Like, I have simulated GCPW with 5.4 mm, I get the phase of 107, but when I simulated 10.8 mm which is a multiple of 5.4mm I get the phase difference of 145 rather than 107+107=214 degrees and so on. I also attached my presentation with this question.
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Notice that the longer line exhibits a phase transition at 8.4 GHz from -180 to +180 degrees. If you linearize the plot by subtracting 360 degrees for all responses above 8.4 GHz, the phase at 10 GHz becomes 145-360 = 215 degrees, very close to the 214 degrees you expected. The circuit is simulation responding normally.
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I am designing two RF tracks (Transmission lines) based on Grounded Coplanar waveguide. The length of both tracks is same, but there is still a phase difference between two tracks.
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Marina Qasim Yes, the propagation constant of the CPW mode will vary slightly depending on the various conductor/spacing geometries.
If you are seeing this difference in simulation, for lines that should be identical, it could be an indication that the simulation is not sufficiently converged.
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How do we combine the COVs of two independent, uncorrelated variables of different probability distributions?
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Problem Statement:
Weather-related loadings on electrical transmission lines involves incidence of wind on an iced conductor, separately and combined. Current US codes require transmission wires and structures be checked for the following load cases:
L1 Extreme Wind (high wind loads on bare conductors, upto 150 mph or 230 kmph)
L2 Extreme Ice (accumulated radial freezing ice, sometimes upto 2” to 4” in thickness)
L3 Combined Ice and Wind (¼” to ½” ice with variable winds, usually 20 mph to 40 mph)
Wind speeds are often considered to follow a Weibull or Extreme Value type distributions) while ice is generally known to be a Normal distribution. Some known COVs (coefficients of variation) are:
C1 Ice: 0.09
C2 Wind: 0.18 to 0.20
If one considers the load case L3, as shown in the sketch below, the Resultant of the ice load (V) and wind load (T) – both in force units per unit length of cable – can be expressed as:
Force Resultant R = √(V2 + T2)
Can this vectorial approach be valid for a resultant COV? Say COVR = √(C12+ C22)?
Note: Ice and Wind are totally independent variables and possess no statistical correlation whatsoever.
📷
Equations to calculate ice and wind loads are available in standard textbooks. Wind pressure p (psf) is generally approximated as p = 0.00256*S2 where S is the wind speed in miles per hour.
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There is nothing like "failure" as such. The case involves action of wind on an iced conductor. That's all. I tried deriving equations by separating the effects and COV's of ice and wind but the results were disappointing.
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how to calculate the length of feedline or transmission line of microstrip patch antenna? Is there any particular formula?
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can you share the formulas that we have to use to determine for length of feed line?
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In case there is a ready-made Matlab roll, I will be thankful
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Follow these general steps:
1. Define the Transmission Line Parameters: Specify the parameters of the transmission line, such as resistance, inductance, capacitance, and length. These parameters will determine the behavior of the line during fault conditions.
2. Create a Simulink Model: Open MATLAB and create a new Simulink model. Simulink provides a graphical environment for designing and simulating dynamic systems.
3. Build the Transmission Line Model: In Simulink, use appropriate blocks to represent the transmission line components. For example, the RLC Branch block can be used to model the line impedance.
4. Introduce the Fault: Add a fault element to the model to represent the high impedance fault. This can be done using a switch or a controlled current source.
5. Define Fault Parameters: Specify the parameters of the high impedance fault, such as fault resistance and fault location along the transmission line.
6. Simulate the Model: Set the simulation parameters, such as the simulation time and solver options. Run the simulation to observe the fault behavior and its effect on the transmission line.
7. Analyze the Results: After simulation, analyze the simulation results to understand the voltage and current behavior during the fault condition. You can plot and analyze waveforms, compute fault currents, and observe the fault clearing time.
MATLAB code snippet to illustrate the basic steps:
% Define transmission line parameters
R = 0.1; % Resistance (ohms)
L = 0.5; % Inductance (H)
C = 0.1; % Capacitance (F)
Length = 100; % Length of the transmission line (km)
% Create a Simulink model
model = 'transmission_line_model';
open_system(new_system(model, 'Model'));
% Build the transmission line model
add_block('powerlib/Elements/Branch', [model '/Transmission Line']);
set_param([model '/Transmission Line'], 'Resistance', num2str(R));
set_param([model '/Transmission Line'], 'Inductance', num2str(L));
set_param([model '/Transmission Line'], 'Capacitance', num2str(C));
set_param([model '/Transmission Line'], 'Length', num2str(Length));
% Add fault element
add_block('simulink/Sources/Step', [model '/Fault']);
set_param([model '/Fault'], 'Time', '1.0'); % Time of fault occurrence
set_param([model '/Fault'], 'Before', '0'); % Step value before fault
set_param([model '/Fault'], 'After', '1'); % Step value after fault
% Connect the elements
add_line(model, 'Transmission Line/1', 'Fault/1');
% Set simulation parameters
simulation_time = 10; % Simulation time (s)
set_param(model, 'StopTime', num2str(simulation_time));
% Simulate the model
sim(model);
% Analyze the results (e.g., plot waveforms)
t = simout.Time; % Time vector
V = simout.Data; % Voltage waveform
I = simout.Data1; % Current waveform
figure;
plot(t, V);
xlabel('Time (s)');
ylabel('Voltage (V)');
title('Voltage Waveform');
figure;
plot(t, I);
xlabel('Time (s)');
ylabel('Current (A)');
title('Current Waveform');
```
you can modify the model to include additional elements, such as circuit breakers or protective relays, to study the fault clearing process and the effectiveness of protection schemes.
Good luck!!
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I'm trying to design a tunable microstrip combline filter with its initial f0 at 2.45GHz, with my resonator's electrical length at 45 degrees to provide maximum tuning range. I'm having problems with my CST simulation, where I'm trying to find the unloaded Q-factor of a resonator. I don't trust the results I'm getting (a Q0 of over 1000 for a 18um copper trace on a Rogers substrate, which I thought would be below 300) and am wondering if I'm using CST correctly.
The only thing I think can be wrong with the dimensions is that I might have chosen a PCB with too thin or thick a dielectric thickness. What are some common thicknesses used for applications at 2.45GHz?
The below list is the steps that I've followed. Hopefully something erroneous pops up to someone more experienced than I.
I've set up the simulation for Q0 extraction as follows:
  1. I entered the required parameters: resonator's height, width, length; substrate's height, width, length (based on the resonator's dimensions), and eps_r; the vias' outer diameter and offset from the bottom.
  2. I created the substrate, groundplane, and resonator, defined their geometries, materials, and positions, and placed them accordingly. I then created an airbox and set its position on top of the substrate with appropriate dimensions, and set its material to vacuum.
  3. I then boolean inserted the vias into the substrate, groundplane, and resonator. After this, the resonator and vias were boolean inserted into the airbox. I wonder if the boolean operations I performed were incorrect, as I'm not sure what exact operations to follow in order to ensure proper electrical connections.
  4. I selected the eigenmode solver, used the tetrahedral meshing technique, and defined the frequency ranges.
  5. The simulation was then run: two modes were found, both not at my desired f0 but almost double and 4x respectively, both showing an unloaded q factor of way higher than 300 (which I thought was a practical max for copper on most Rogers substrates).
My goal is to get Q0 at my desired resonant frequency, but the mode frequencies CST gave me is not at 2.4GHz. I don't think it's a fault with the dimensions, but I could very well be wrong. I suspect I might have made a mistake in how I set up my simulation.
Please advise me on any possible errors I could be making, or perhaps better ways of going about the simulation.
I can't seem to find anything on YouTube detailing the process I'm embarking on, nor do the papers I've found detail exactly how they arrived at their filter's dimensions from simulation, they simply provide their resulting parameters.
Thank you for your time.
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How did you implement the resonating capacitances? Depending on earthplane spacing and bandwidth, waveguide modes below cut off can also do funny things.
For coupling factors, etc., Involving two resonators, the resonant frequencies without coupling must be exactly the same if you want to use the standard equation for coupling factor [k=(fo^2-fe^2)/(fo^2+fe^2)].
R.Levy published several excellent must-read articles on comb line filters.
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What is the most recent technique used in mitigating transmission losses?
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EHV transmission is limited by increased lines capacitance as C= dq/dv, HVDC the best with advent in semiconductor technology for converters and inverters…..
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Which readily available simulator can i use for lightning simulations on Transmission lines? also how do i perform, the simulations?
Im doing a tranmission line upgrading project and i need to make sumlations to that effect
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Where can I download these free programs from?
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I am implementing a microstrip band-pass filter with high-low impedance sections (stepped impedance). The impedance is varying between 12ohm and 182 ohm, Zmin, Zmax respectively. For lowest impedance section 12ohm and other Z values (typically below 100ohm), when i simulate these individual sections of strip in CST, the simulated line impedances are almost same as required. For highest impedance 182-ohm transmission line required minimum strip width is 0.100 mm. I used the Lincalc from ADS to extract the corresponding substrate h (for 182ohm, 0.100micron w) which turn out to be 2.4mm at 11.75GHz (center frequency), 9.15 epsilon. When I simulate this w,h (0.100mm,2.4mm) in CST to verify the 182ohm, the simulated line impedance give a value of around 90ohm. It happens to all Z values higher than 100ohm. The problem in S-param are the return loss, the required RL is 20dB but the simulated one is around 12dB. I want to know if high impedances (Z>100ohm which are not achieving in simulated case) is contributing in worse RL or there are other factors. If this is about high impedance section, then how i can implement it to achieve the desired 182 ohm.
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Yes, I agree with @Malcolm White, But if still want to design a high impedance transmission line, then you need to learn SISL technique.
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SIL is define as when transmission line loaded with Impedance equal to its Surge Impedance ignoring Resistance and conductance. When Surge impedance is equal to load impedance the sending end and receiving end voltages are equal.
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Standing waves can occur in transmission lines at power system frequency under certain conditions. When a voltage wave travels along a transmission line, it encounters a load impedance at the end of the line. If the load impedance is not matched to the characteristic impedance of the line, a portion of the voltage wave is reflected back towards the source. This reflected wave can then interfere with the original wave, resulting in the formation of standing waves.
The formation of standing waves in a transmission line is influenced by various factors, including the length of the line, the characteristic impedance of the line, the load impedance, and the frequency of the voltage wave. In particular, the relationship between the load impedance and the surge impedance of the line can affect the likelihood and severity of standing waves.
The surge impedance of a transmission line is the characteristic impedance of the line when it is assumed to be infinitely long. When the load impedance of the line matches the surge impedance, there is no reflection of the voltage wave, and standing waves do not occur. However, if the load impedance is higher or lower than the surge impedance, some of the voltage wave is reflected back, leading to standing waves.
In summary, standing waves can occur in transmission lines at power system frequency, and the relationship between the load impedance and the surge impedance of the line can affect their formation.
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Hello
I want to design a riblet hybrid coupler (Short Slot Hybrid Coupler) in X-band.
1- What should be the length of the couple region, the distance between the two common walls?
2- What techniques can I use for phase shift?
If you know an article or book in this field, please introduce it
Thanks
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Hello dear friend, thank you
According to the article:
Do you think it is easy to use the thesis of trapezoidal dielectric shape in reality?
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Suitable compensator upto 500KV ac transmission line, where power level will increase for modern era with affordable cost.
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The best solution depends on the faced criticalities, e.g. voltage regulation, transient stability, power bottleneks and so on. At 500 kV level shunt reactors are generally required. In case of long lines, series compensation is widely adopted. In particular series devices directly impact on power transfer. Controlled compensators, i.e. SVC's, STATCOM's, TCSC's, SSSC's are expensive, nevertheless are steadily penetrating in power system. This also because of the operation flexibility they offer.
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In the MATLAB simulation model of any power system model taken from www.mathworks.com, the parameters of power system components like generator, transformer, transmission line, load etc are set according to 60 Hz american standard, how to convert parameters of all power system equipments from 60 Hz american standard to 50 Hz european standard. Is there any procedure or empirical formula for this ?
I just want the clue or idea. I am not asking for an exact answer ?
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All power system equipments working at designed constant flux density or could say constant V/f ratio. The iron loss of equipments consist of hysteresis and eddy current loss which depending on frequency or Wi=Wh+We=A(f)+B(f)(f), or though cooper loss could be same of equipments but the iron loss would increased with increased frequency. Method to find A and B constants of given transformer is explained in my answers….
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Hello,
I am using CST Studio to simulate an interdigital capacitor and to extract its S-parameters of it. in order to process those measurements and obtain the parasitic elements that it contains. However, when I calculate the equivalent capacitance and inductance of it, it has negative and imaginary values, which do not make any physical sense. Therefore, I wanted to know if I was simulating it in the correct way. I put two ports, one in the input, and another one in the output and I put all the boundary conditions in 'open'. About the ports, I calculated the microstrip ports using the CST macro. I have attached a picture of the design to make it more clear. (perspective, top and bottom view).
My question would be: Should I use these boundary conditions? Is this the correct way to put the ports? Should I do any modifications to obtain a coherent result?
Best Regards
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you may treat it a printed strip-lines or perhaps microstrip lines depending on your ground plane and a possible cover plane adn the evaluate S11 vs frequency. Make sure that it cannot radiate
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I face a very lossy line (cryogenic harness) with L = 320 nH/m, C = 60 pF/m and R = 10Ω/m characteristics. I can estimate the characteristic impedance of this transmission line as Z0=√L/C~70Ω. with 2 meters length, the lossy part is about R = 20 Ω. My simple question, is, if I want to amplify the end of this line with a good input matching, what LNA input impedance have I to match ? Z0 line impedance ? Z0 "+" R line impedance "+" resistance? Source impedance Rs? Source impedance Rs + losses R?
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Hello! The expression √(L/C) is correct just for the determination of the characteristic impedance of lines with negligible losses. Try to use a complete formula that contains also dissipative parameters.
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why the series compensated transmission lines connected to hydro power stations don't face the problem of subsynchronous resonance but the series compensated transmission lines connected to thermal or nuclear power stations or wind power stations faces the problem of subsynchronous resonance ?
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Series compensated transmission lines that are connected to hydroelectric power stations typically do not experience the problem of subsynchronous resonance (SSR) for several reasons.
First, series compensation (the use of capacitors or reactors in series with the transmission line) can help to stabilize the transmission line and reduce the risk of SSR. Series compensation can reduce the line impedance and increase the system damping, which can help to suppress the oscillations that can lead to SSR.
Second, hydroelectric power stations typically have relatively low inertia and fast-acting governors, which can help to dampen oscillations and reduce the risk of SSR. The governors of hydroelectric power stations can quickly respond to changes in system frequency and adjust the power output of the station accordingly, which can help to stabilize the system and prevent the development of oscillations.
Finally, hydroelectric power stations are typically operated in a load-following mode, which means that they can adjust their power output in response to changes in demand. This can help to dampen oscillations and reduce the risk of SSR, as the system frequency is less likely to be disturbed by changes in load.
Overall, the combination of series compensation, low inertia, and load-following operation can help to reduce the risk of SSR in transmission lines connected to hydroelectric power stations.
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As I mentioned above reviewer has asked me to make changes, like write down complete details about faults in the smart grid though my paper is about faults in transmission lines. My paper already has 12 pages if I add those irrelevant details it will increase the number of pages also. And another thing he has asked to merge all graphs which I think will make it too much complicated for reading. So how should I deny those changes which will not a kind of "offened" the reviewer?
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Just try to do everything the reviewer asks because it will make the process easier :)
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What would be the possible dangers of using neodymium magnets near High voltage transmission lines or other high-voltage equipment? Is there any method by which we can make it safe to use?
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Any magnet could be effected by flux produced by current voltage with in break down insulation would not effect the magnetism of magnet….
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Hello good time
What metals can be used in the design of high frequency devices such as Coaxial transmission lines , waveguides, coaxial to waveguide adapters? (Diamagnetic, paramagnetic or ferromagnetic)
For example, can I use tungsten rod , which has a magnetic permeability coefficient of 1, to build a coaxial transmission line? (What is the appropriate magnetic permeability number for the metal used to have low insertion loss(S21)?)
Thank You
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Fundamentals of microwave and RF Design by Michael Steer, NC State.
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As the title says I am curious about whether the line transposition (eg - 1/3-1/3-1/3 transposition scheme) affects the behavior of fault-induced transients compared to an ideally transposed transmission line.
Is there any literature that has analyzed this topic?
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Dear Sir, I refer the general output of extensive studies performed about 50 years ago on the Transient Network Analyzer. The results obtained with a continuously transposed model are close with those obtained by an asymmetrical model with full transposition as you mention. This refers to a generic study. When attempting to reproduce a specific transient recorded in the network the actual transposition scheme (with many other details) should be considered. By the way the 1/6-1/3-1/3-1/6 scheme is preferable since it doesn't affect the physical position of the phase conductor in the stations.
Moreover, the above reported general conclusion applies to a single circuit transmission lines. When the coupling between parallel circuits is present (say two circuits on the same support or in close proximity) the differences of the results obtained by the continuously transposed model and the asymmetric model might be large.
As regard the literature references, I remember that there were some working documents of CIGRE WG groups 13-05 and 33-02 in early seventies. In those days there was also a symposium at UMIST organized by prof. Bickford on transients produced by faults. May be you can find something.
Best regards, Giulio Santagostino
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i understood that every coaxial transmission line has a cut off frequency.
it seems strange to me, because the real behaviour of a transmission line in every frequency base on its equations is a delay time! so why the transmission line has a cut off frequency?
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A coaxial transmission line can operate with different field patterns in it. The most simple is when the electric field is radial from the middle conductor to the outside conductor. This is called the fundamental mode and is a TEM mode and works down to DC and up to any frequency. The wave will travel at the speed of light that is expected in the dielectric that fills the gap.
There are other patterns that are possible, such as with the electric field being upwards at the top, and also upwards at the bottom, and zero to the right and left sides of the centre conductor. This mode will not carry power along the line until the mean circumference of the gap is close to one wavelength in the dielectric filling. The frequency corresponding to this wavelength is called the cutoff frequency for that mode. The cutoff frequency is usually thought of as a lower frequency below which that mode doesn't propagate. There are other modes, with more complicated, patterns, for which the cutoff frequencies are even higher. Actually there are an infinite number of higher modes!
The cutoff mode for the first mode above the TEM mode is the upper cutoff frequency for safe use of the TEM mode, because above this frequency bends and steps and joins can generate other modes which travel at different (slower) speeds and can result in signals getting scrambled.
Below cutoff, a mode doesn't carry power, but the field from it, if you try to send it into the coax, or accidentally create it at a step or bend, looks like the field of an inductor or capacitor, and falls off very quickly along the waveguide. At frequencies only just below cutoff, these may actually go quite a long way along the guide, and seem to appear at the other end with no time lag, just as the inductive near field of a coil seems to increase immediately a small distance away from the coil, each half cycle. This immediate response can only be seen in simulations, where seeing the fields doesn't affect them. As soon as you use something to detect the real fields, it absorbs some power and changes the fields and a time delay is measured.
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I am working on transmission lines, so i decided to simulate the real delay of electromagnetic waves in a cylindrical transmission line. base on my calculations and formulas, the delay of a wave in a 1 meter oil filled transmission line is 5ns , but when I simulate this simple structure in CST MICROWAVE STUDIO, I see a wrong time delay about 1 ns. so what do you think about this bug?
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You may have been launching a higher-order mode which was cut-off but not far from its cut-off frequency, so the exponential fall-off length was quite long, resulting in strong evanescent (inductive) fields at the far end.
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Where are PMUs installed exactly at the electric grid? at the substation level or transmission lines? is it possible to have PMUs at Distribution Level as well?
Thanks
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PMUs are installed at sub-stations at the transmission or distribution levels. PMUs installed at the distribution sub-stations, usually have a higher refresh rate as compared to that of the transmission sub-stations. We call them DPMU or micro-PMU.
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I'd like to address one of my concerns regarding multiline TRL calibration. After calibrating a frequency, I occasionally did not get the expected result. If you look at my attachment, you'll notice that after calibration in some frequency ranges, it shows a sharp curve above 0dB (sometimes). Is there anyone who can say me why this type of error occurred?
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This is the typical signature if a bad contact (loose connector) somewhere in your setup
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what are parameters required to prove an SSPP Transmission line?
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A dispersion diagram is a plot of frequency (usually in radians per second) on the vertical axis, against wavenumber (usually in radians per metre) on the horizontal axis. In vacuum it is a straight line through the origin and the slope is the speed of light. In other materials it is different to this. The speed may not be the speed of light and may vary with frequency. The local gradient is equal to the phase velocity, which is the speed the pattern of electric or magnetic field can be measured to travel (like Moire fringes), and the ratio frequency/wavenumber is the group velocity, which is the speed that information or power travels.
If the material is periodic, the pattern repeats itself, along the horizontal axis, and the diagram only shows one period. It can be different in different directions, and sometimes one period in the x direction is plotted, followed by one period in the y direction then one period across the diagonal.
I don't use HFSS so can't help with that.
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Below pictures are my design of a transmission line, for this simulation I set driven terminal. As you can see one side of the transmission line is differential pairs, another is single ended. If I want to see insertion loss of the transmission line how should I set the rectangular plot? Set "Show" to terminal and see St(Tline_T1,Tline_T3) and St(Tline_T2,Tline_T3) respectively? or set "Show" to differential pairs to see St(Diff1,Tline_T3)? or other?
Is it St(Diff1,Diff1) for return loss?
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Thanks, that makes sense.
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I am trying to design a CPW-GCPW tapered transition. Can anyone recommend a book or a reference for these types of transition structures? (Like how to calculated the tapered length etc.)
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The catch for the design of such kind of structures is the right combination of protein and silicon computers; the silicon computer in genal will not tell you the shape you should use..but once you have a shape in mind you can nicely analyze it in great detail which is not to easy for the protein computer (your brain); there are many books which discuss tansitions of all kind..but the gernal rule it..avoid sharp steps and try to implement for or less smooth transients from one cross-section to another...use you intuition there...and then ask he silicon computer jow he likes this.
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According
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Average 3 period
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I've included an example picture. Is this transition followed by Quarter Wave transfer rules? or, Can anyone assist me in properly identifying this transition section?
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You should know that this is not governed by quarter wave transition rules. A quarter wave transformer transforms between two different impedances not two impedances that are the same. The flare will introduce an effective lumped capacitance at the join and may be to compensate for other parasitic inductance or capacitance at the transition.
It probably isn't, but it may just be a badly designed transition. Not everything in published papers is good, especially if that wasn't the main point of the paper.
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If we connect the top and ground metal layers with a lot of Via, will the parasitic capacitance increase or decrease? As far as I know, it will reduce resistance.
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Hi
Having too many Via in PCB can introduce significant parasitic capacitance. If it is known that the diameter of the solder mask on the ground layer of the via is D2, the diameter of the via pad is D1, the thickness of the PCB is T, and the dielectric constant of the PCB board substrate is ε, the parasitic capacitance of the via is approximately C=1.41εTD1/(D2-D1)
The main effect of the parasitic capacitance of the via hole on the circuit is to extend the rise time of the signal and reduce the speed of the circuit. In addition, the smaller the via, its own parasitic capacitance. The smaller, the more suitable for high-speed circuits.
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Like the power transmission systems have transmission lines that carry impedance/admittance and this power transmission network can be seen as a graph with edges having weights as the admittances. Do the feeders in the distribution networks carry admittances that can be seen as edge weights?
From an admittance bus matrix one can construct a power network with buses connected with the transmission line having the admittances (being the entries of the bus matrix). Can this similar method be applied on feeders connecting busbars in a distribution network.
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As name suggested transmission lines are transmitting power mainly from generating stations to distribution stations and are three phase three wire in system, transmitting by step up transformers from few KV to 66KV or higher even EHV or HVDC as needed via circuit breaker, CT, PT, and lightening arrester to line and receiving at step down transformer via lightning arrester, CT,PT, and circuit breaker to step down transformer at distribution substation, at load area.
Distribution feeder are using three phase four wires system supplying three phase or single phase via pole mounted transformers from step down transformers secondary side busbars from, few KV, to rated Voltage needed for industry or domestic via pole mounted transformers, distribution of load should be maintained balance for better system efficiency and to reduced neutral current. Though feeder system admittances are generally, not considered in load flow analysis and calculations for simplicity…..
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Why the fault current ?
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I think this is because the energy transfer takes place at sub-synchronous frequency (below 50Hz) unlike the normal case at 50Hz, and thus the energy flow (power (voltage and current)) all look distorted.
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Firstly, thank you very much for reading this question!
Now I am designing a T junction build-up with the transmission line. I find that I have to design this T junction within a dimension less than 1/4λ, but I have seen that I have to consider the transmission line effect when the electrical line pattern is >1/4λ (someone even says> 1/10λ), and I do have seen some transmission drops for my interested band in simulation, seems like I have to do something with impedance matching.
Usually, we have those impedance matching schemes with 1/4 λ length(Quarter-wave impedance transformer), but they are too long for me. My question is, do we have any choices that we can achieve impedance matching with a smaller size impedance transformer?
Thank you all very much for the information and the ideas!
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If the lambda/4 option is too long, I assume you work with relatively low frequencies. A transmission line which is close to lambda/4 length is indeed masking quite a lot the load impedance (I tend to agree with the > 1/10λ criterion). For this range of problems, I would look at LC matching boxes. According to the load value, you can choose the type of LC circuit (L series and C parallel, for example) to design and the related values. These will work only for that load value, and only for that frequency.
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I am
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I am
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If there is enough train data for all fault type cases to clamp to input and output, there will not be a need for a fixed threshold.
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Can anybody
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We
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Siddharth Kamila Subsynchronous resonance is a phenomenon in which one or more of the resonant frequencies of the turbine generator shaft in thermal power units coincide with a natural resonant frequency of the electrical system with a long radial transmission network with series capacitors, resulting in a voltage drop.
Sub-synchronous control interaction (SSCI) is a stability issue induced by the interaction of a doubly-fed induction generator's control system and a series-capacitor compensated electrical network. It might cause system instability if not addressed appropriately.
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I have trained trtbgdfdh
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Dear Siddharth Kamila:
You can benefit from these valuable Link about your topic:
##################
Also you can take a look at:
"Fault Detection of the Power System Based on the Chaotic Neural Network and Wavelet Transform"
Abstract:
The safety and stability of the power supply system are affected by some faults that often occur in power system. To solve this problem, a criterion algorithm based on the chaotic neural network (CNN) and a fault detection algorithm based on discrete wavelet transform (DWT) are proposed in this paper. MATLAB/Simulink is used to establish the system model to output fault signals and travelling wave signals. Db4 wavelet decomposes the travelling wave signals into detail signals and approximate signals, and these signals are combined with the two-terminal travelling wave location method to achieve fault location. And the wavelet detail coefficients are extracted to input to the proposed chaotic neural network. The results show that the criterion algorithm can effectively determine whether there are faults in the power system, the fault detection algorithm has the capabilities of locating the system faults accurately, and both algorithms are not affected by fault type, fault location, fault initial angle, and transition resistance.
I hope it will be helpful...
Best wishes...
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case1 : when Radio frequency wave transmision line is loaded with matched impendace, then entire signal is taken by load without any reflections..
case 2: when a Radio frequency wave transmision line is loaded with short circuit, then entire signal is reflected back...
Now what happens when both the above cases are combined?
where will the signal go and how much will be the reflection coefficient?
will the matched impedance load get any signal?
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Yes, the signal will be reflected back and ods not reach the load. At the opposite end, the load will see some impedance varying from short to open depending on the electrical length of the transmission line between shorted point and the load.
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I have written code for MTL model in MATLAB by referring an authors paper. The correctness of the waveforms obtained in time domain in MTL model depends on the data being used, which shouldn't be the case. For some data I get correct waveform , for others it gives absolutely erroneous result. I am not able to figure out where it might be going wrong. Could someone please guide me regarding this. Its been really long , I am trying to figure this out.
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Hi,
it is hard to answer your question without knowing which model you want to code, and the code...
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Unfortunately, this simplistic vision of RF and microwave circuit design often becomes blurred when test results are obtained that differ drastically from the beautiful simulation results. The reasons for this disparity may normally be traced to one of the following:
"The ratio of the transverse dimensions of transmission lines to wave length are nonnegligible thus, additional unwanted energy storage modes become available."
I read this above paragraph in a textbook, and didn't quite understand the sentence given in bold.
As of how does the above condition result in unwanted energy storage modes.
Thank you in advance
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As one example (I think)
Microwave waveguides are usually used in the regime where the widest width of the waveguide is less than a free-space wavelength, and more than a free-space half wavelength. This means that there is only one way, or mode, in which the signal can travel down the guide. If the guide is wider than this it becomes possible for energy to travel down it in multiple modes with different velocities, and, even if only one mode is launched, other modes can be generated at bends and other components.
Even in the usual regime, the signal (group) velocity depends on frequency.
Also, at things like steps in the waveguide walls, modes can be generated even when the guide is less than a wavelength across. In the case of the guide being less than a wavelength across, these do not propagate but store energy similar to inductance or capacitance, and the stored energy may be larger for larger guide sizes.
All of these result in more complicated behaviour than a simple ideal transmission line, and happen because the time taken for the signal to travel between opposite conductors is not minute compared to the time taken for the signal to reverse in the transmission line.
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Power Network Expansion Planning is the problem of deciding the new transmission lines that should be added to an existing transmission network in order to satisfy system objectives efficiently. It is one of the main strategic decisions in power systems and has a deep, long-lasting impact on the operation of the system. Several challenges such as deregulation, renewable penetration, large-scale generation projects, market integration, and regional planning are discussed in the literature to some extent.
In the context of the smart grid, what can be the potential future challenges in terms of different scenarios, applications, modeling, solution, and novel devices in the network?
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Two main problems in the perspective of SG:
*Integration of Microgrid, while considering uncertain factors and limitations of the present grid.
*Integration of charging stations for EVs taking into view users' profiles and traditional grid capacity.
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Hi,
I am trying to plot the dispersion diagram for a transmission line metamaterial IFA antenna, consisting of a capacitor in series and an inductor in parallel to the antenna.
As far as I know, the dispersion diagram is the plot of frequency vs. phase of S21, as phase (theta) is beta*length.
But how to plot the dispersion diagram of an antenna which has only one port?
Kindly help me!
With Regards,
Suhas D
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Thank you Madam Aparna Sathya Murthy and Sir Stuart Barth for your help.
I was going through a paper titled "Small Antennas Based on CRLH Structures: Concept, Design, and Applications."
In this paper the authors have come up with the dispersion diagram of a 3 cell metamaterial antenna (please find attached the image). But I don't understand how they got it. This is the kind of dispersion diagram I need for my metamaterial IFA antenna to observe the Right Handed and Left Handed regions.
Any ideas? Please do help!
With Regards,
Suhas D
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I would be glad if there's any way of finding the capacitance per unit length. since SIMULINK parameters block critically requires at least nearest values of all resistance, inductance, capacitance to get proper output results.
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Capacitance is missing in many data sheet of low voltage cables since it doesn't practically affect the cable performances at power frequency. Yuo may find in the literature data. e.g. : Geis-Schroer, J.; Hubschneider, S.; Held, L.; Gielnik, F.; Armbruster, M.; Suriyah, M.; Leibfried, T. Modeling of German Low Voltage Cables with Ground Return Path. Energies 2021, 14, 1265. https://doi.org/10.3390/en14051265.
As a crude approximation, you can consider the relative permittivity of the insulation, say 4.8 for PVC, 2.8 for XLPE. The specific capacitance is C=eps /L/c^2 where L is the associated high-frequency specific inductance, c is light velocity in vacuum. In fact you should consider that in three-phase circuit different capacitances exist. The shields and the armouring (if any) affect the capacitances.
Best regards. Giulio
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if we have a simple power system that consists of two generators and a one transmission line. One generator is operating at 50 Hz, and the other one is operating at 51 Hz. X is the line reactance, ignore line resistance. 
a)      What will be the nature of power flow P? If both generators have same voltage magnitude and the same phase angle?
b)       What will be the nature of power flow Q? If both generators have same voltage magnitude and the same phase angle?
c)     the generators have the same voltage magnitude but have different phase angle.
d)      the generators have the same voltage magnitude but have different phase angle.
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Dear Irfan Khan,
The load angle is difference in angle between induce EMF and Terminal voltage.
Now , we know that phase angle of voltages with phase A,B,C are 0,+120,-120 degrees.
Now when we add load to the alternator the terminal voltage will lag the induce EMF so these angles will change?
If these angles will change then this will effect p.f. power factor is cosine of angular difference between voltage and current but if phase angle of voltage changes then this effects power factor or angle of current will change accordingly?
If we want to synchronize two different alternators having same freq but with kva ratings then load angle will not be same then how does power transfer efficiently .
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I want to generate a sinusoidally varying impedance transmission line for the following specifications:
min. impedance 50ohm, max. impedance 170, period 10mm
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You could do this in stripline or microstrip by changing the width of the track.
This would be called an impedance modulated grating, an will cause frequency dependent reflections. Microstrip filters can be very similar to this, with small variations to the periodicity to improve the performance.
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I welcome all to this discussion.
Generally, we say that the algorithm giving fault location error of less than 5% is ok and lesser error indicates the superiority of the fault locator algorithm. Is any IEEE or other standard defines the limit of fault locator error?
This question is in the context of the transmission line protection.
Thank you for your time.
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In the standard of Rosseti FGC UES (Russian energy company), the following errors are claimed:
1. ±1 % - for double-ended fault location;
2. ±2,5 % - for single-ended fault location.
Errors are claimed for 50 Ohm fault resistance.
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I want to design HVDC transmission line for simulation purpose in MATLAB but dont know how to set different parameters values any idea how can I do that? any artical/website/book from where I can learn that.
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You may find useful information and examples in CIGRE Technical Brochures 368, 492, and 831.
Best regards, Giulio Santagostino
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Hi, I need a power system model with 2 - bus, 2 - machines and a long-distance HVAC transmission line.
Would you mind providing with me all the necessary parameters of the system?
Bergeron line models will work for me.
Your help is greatly appreciated.
Thank you
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There is a book "Power System Stability and Control" Prabha Kundur has simple networks
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The above model is useful in studying and testing the distance relay when a fault occurs at 75% of the length of the line because the line is divided into four equal parts.
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Dear Bashar
So I am, I agree with Pablo Gómez
Best regards
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Good day everyone. Is the Normalized Standard Deviation only parameter for measuring the accuracy of the Multiline TRL?
  • Is there any other way to show the effectiveness of Multiline TRL?
  • Also, could someone explain what Normalized Standard Deviation is and how it is calculated?
Thank you in advance to everyone.
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Dear Qamar Ul Islam Thank you for your reply. Actually, all of your suggestions are related to the field of chemical and environmental engineering. My scenario is related to wireless communication, and I can include an example to you: https://ieeexplore.ieee.org/stamp/stamp.jsp?arnumber=85388
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Hello,
I'm designing a CPWG in the 30 GHz range in HFSS. I noticed that in my design the characteristic impedance is variable across my simulation range from 15-50 GHz. I think this is to be expected but more importantly the impedance of the line seems to be quite sensitive to the port definition. If I use the suggested wave port width the port overlaps with the coplanar grounds and the impedance drops from 52 ohm to 14 ohm. Any suggestions or tips on how to accurately do this and ensure no artifacts from the wave-port definition?
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In CST it is possible to look at the port mode fields that have been calculated. It probably is in other codes. Keep making the port bigger until the fields stop spreading wider when you make the port bigger. Also keep making it bigger until the port impedance stops changing.
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Hello, Here is my microstrip transmission line CST file which has been created by the Macro->calculated-> calculate analytical line impedance with these parameters Er=3 H=.6mm W=1.5mm L=10mm Frequency=5Ghz
But the S11 and S21 are not acceptable. I need to know what my problem is.
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How are you feeding it and terminating it? You should be using waveguide ports. They need to go down to the ground, about 3 to 5 line-widths each side and at least that much in the air above.
What is your dielectric and what are your conductors? How long is the line? Your insertion loss is not just unacceptable, it is ridiculous, unless the line is 100s of metres long.
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Hello,
I need to know why shorter impedance matching(IM) transmission line has higher Band width? (for example in designing IM circuit which has been calculated by Smith chart the shorter solution is preferred because of higher band with).
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So The term “impedance matching” is rather straightforward. It’s simply defined as the process of making one impedance look like another. Frequently, it becomes necessary to match a load impedance to the source or internal impedance of a driving source.
Sir i think you could benefit from this valuable articles about your topic at:
1-- https://www.electronicdesign.com /technologies/communications/article/21796367/back-to-basics-impedance-matching-part-1.
2-- https://studylib.net/doc/25266752 /chapter-3-impedance-matching.
Information about (Stub tuners) - as you know - are basic laboratory tools used for matching load impedances to provide for maximum power transfer between a generator and a load, and introducing a mismatch into an otherwise matched system. Typical applications include power and attenuation measurements, tuned reflectometer systems and providing a DC return for single-ended mixers and detectors.
Stub tuners are impedance transformers that are designed to introduce a variable shunt susceptance into a coaxial transmission line. They consist of one or more short-circuited, variable length lines (stubs) connected at right angles to the primary transmission line. Each stub must be movable over one-half wavelength at the lowest frequency of operation in order to provide all possible shunt susceptances; therefore, the low frequency limit of a tuner is determined by the frequency at which the maximum stub travel equals one-half wavelength. Tuners, particularly multiple-stub models, are still usable below this limit. Other than the limitation of the connectors, there is no higher frequency limit; however, various models are offered for size convenience.
The spacing between the stubs of multiple-stub tuners determines the range of impedances that can be matched and the ease of tuning . The stub spacing of Maury double- and triple-stub tuners has been selected for general broadband applications. Triple-stub tuners are more convenient to use since tuning sensitivity is relatively independent of stub spacing.
Maury produces a comprehensive line of broadband stub tuners designed to satisfy the majority of applications. These tuners are available in double- and triple-stub configurations with frequency ranges extending from 0.2 to 18.0 GHz.
I hope it will be helpful...
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I am working on developing a model for transmission line failure in power gird. I need some information about capacity of each transmission line of IEEE 300-bus test case to identify lines that exceed their capacity (power/voltage/current). I couldn't find any data in the reference model.
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The official documentation does not include limits for all nodes and branches, for reference you can follow those in Table E.1 (for bus voltage limits) and Table E.2 (for branch loading limits) in:
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Power system equipment needs periodic maintenance services for reliable operation with a lower forced outage frequency.
Maintenance scheduling is a program that optimally schedules the preventive maintenance for generation units and transmission lines. Through this program, the benefit of generation units and transmission lines, as well as the power system reliability, are taken into account simultaneously. Such programs maintain the system reliability by considering the simultaneous maintenance of power system components (particularly in low-price time periods of the year when generator owners want to temporarily keep their facilities out-of-service for maintenance services). Accordingly, preventive maintenance has different advantages as:
- Reducing failures frequency that prevents the reliability deterioration of the power system, particularly in both low-demand (decreasing the number of under-maintenance components) and high-demand (decreasing the forced outages of units) time periods
- Improving repair costs
- Retaining the useful lifespan of facilities
What other benefits are there for preventive maintenance?
Thanks
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Would reduced the life consuming cost, would increased the generating and transmitting efficiency, would reduced the temporary faults, increasing reliability of power system. Short time overloading could also be increased, refer my papers on short time over loading utilizing remaining life of a day……
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Hello everyone
Recently, I've been working on constructing the waveform for the simple PCB interconnect by means of existing algorithm, which means I don't want to use the commercial software.
To be simple, I suppose the topology is just TX + transmission line + RX (See Fig. 1)
At the beginning, I just wanted to quickly estimate the waveform with ideally initial waveform (See Fig. 2)
Unfortunately, I had no idea to estimate the TX output impedance and RX input impedance.
Eventually, I thought I had to build the waveform by means of interpreting the IBIS models.
There are [Pullup], [Pulldown], [POWER Clamp], [GND Clamp],... in the IBIS.
However, I don't know how to use them to construct the waveform and get the internal impedance.
My question : How to do that with the IBIS information?
(Suppose the IBIS is 4.2 version)
Thanks for your kind reading.
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Sir Szuhsien:
You are welcome, and i wish you good health and happiness....
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Is XLPE best insulator material for Medium Voltage underground electrical cables for Transmission Lines?
Normally the rated operation temperature for XLPE at this applicaction is 90 °C, So the temperature is not an issue , but what about the weight, cost and amount of material required for one meter of insulated Aluminum/Copper
Thank You!
Best Regards !:)
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I am doubtful on the replacement of XLPE in such a short period. Some European companies are claiming that they are recycling XLPE. Apart from this, on account of much lower loss factor XLPE is likely to continue as a leader for some more time.
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What is the maximum and minimum frequency in which a microstrip transmission line can operate without distortion for a particular length and width of the trace?
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If you want to know the effect of microstrip on signal integrity, you need to consider bandwidth, not just frequency. Microstrip is dispersive, so all signals except CW will become spread out over distance.
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I need to calculate the values of R, X, G and B used in the t-model of the transmission line.
I have a 4 core wire and its data sheet, ( https://www.hesselmann.de/data-download/produktinfo/he-nycwy.pdf ).
How can I derive these values from this data?
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Hello.
I could not figure the cable layout based on the datasheet you provided, but my best bet would be the Line/Cable Constants routine from EMTP/ATP, modeling a combination of cables with an enclosing pipe. I suggest you have a look at: https://www.atpdraw.net/help/model_data.htm
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I have been trying to implement Multiconductor transmission line(MTL) model for the transformer winding and then apply Numerical Inverse Laplace transform to get the time domain response in MATLAB. The equations I am using for MTL modelling are given in the paper attached below. The response I get doesn't match with the response given in the book. I am not able to figure out in my MTL code as to where is the mistake? Am I applying the MTL equations incorrectly or NILT is going wrong somewhere. Can someone please guide me regarding MTL modelling? Which equations are correct ?
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Relation between electrostatic based problem and time harmonic electrodynamics problem.
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Dear Thomas Cuff, my doubt is for the analysis of the time-harmonic electromagnetic field, how can we take electrostatic behavior like inductance and capacitance into account. As the field behavior is completely different and wavelength is comparable with the physical dimension of the device, is it sufficient by considering capacitance per unit length or inductance per unit length? Whether we can calculate the field correctly by this approach.
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Recently, I'd like to collect some formulas for some specific transmission line structures in PCB (single-ended stripline, single-ended microstrip line, etc)
I found that there is no formula related to the impedance of the microstrip line with solder mask (the region above the solder mask treated as the vacuum or the air)
Is there any suggestion to find that?
Thank your reading
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In this case case I would go for a numerical evaluation which is rather easy these days..even if there is a formula somewhere it will be an approximation and not straightforward to solve
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R & X is ohm/km.
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The basis for knowing the value of the maximum power flow of a transmission line is to know the value of the surge impedance.
Surge Impedance Loading is a very essential parameter when it comes to the study of power systems as it is used in the prediction of the maximum loading capacity of transmission lines.
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Hello everyone.
I want to research an s-parameters result of a dielectric cylindrical rod in CST software. which port can be used for full dielectric rod or full dielectric transmission lines?
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The waveguide port will match the propagating mode in the dielectric cylinder or transmission line. The discrete port and wires won't.
Only use the discrete port and wires if that is the way the actual circuit will be built.
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I am trying to construct a microwave spoof plasmonic transmission line in CST. In particular, I intend to replicate the results of the paper, Broadband and high-efficiency conversion from guided waves to spoof surface plasmon polaritons. (https://doi.org/10.1002/lpor.201300118). I designed the unit cell in CST. I thought that using VBA macros, I would be able to copy, paste, translate, and boolean add my unit cells, to get the entire transmission line. However, this method didn't work. I am currently trying to design the transmission line in Autocad and import it to CST. I am hoping that it works. Still, I wanted to know if there are any other ways to do this. Thanks in advance!
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Dear Anuvab
first I would make a small remark..I observe with a smile that certain people keep inventing impressively sound names for simple and old stories. The structure and the type of surface wave you are talking about is basically nothing else than a corrugated waveguide with a surface mode that decays exponentially in transverse direction to the propagation. There is a very nice paper on this by E.G Neumann (1968) Elektromagnetische Oberflächenwellen (electromagnetic surface waves).The physics and equation for this type of surface wave are probably already known since nearly 100 years (or more) [Zennek wave, Harms Goubeau wave etc).The way to excite them is a simple horn antenna and you may copy paste the setp from Neumann nice paper..
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I have dataset which shows the length of power lines. I need to classify the lines based on the line length. Is there a rule to classify the High voltage (HV) and low voltage (LV) lines based on line length? For instance, can we say lines below 500m (meters) are considered as LV lines and lines above this length are HV lines?
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Dear Mr Muhammad Ali
You were about to hit the target but missed for just a little bit. Here is the answer to your question in brief.
Transmission lines are classified into two standards.
  • Voltage Rating
  • Length of Line
As per voltage rating, there are 5 types of transmission existing
  1. Low Voltage (LV) < 1000V
  2. Medium Voltage (MV) 1000V < V < 69kV
  3. High Voltage (HV) < 138kV
  4. Extra High Voltage (EHV) 345kV < V < 800kV
  5. Ultra High Voltage (UHV) > 800kV
As per the length of the line, there are 3 types of transmission existing
  1. Short Transmission Line < 50km
  2. Medium Transmission Line 50km < L < 150km
  3. Long Transmission Line > 150km
Once again these standards can vary in different countries. Hope that information will be helpful for you. Good Luck!
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In strings, standing waves of particular frequency is possible only at specific length of string. But in transmission lines, no such conditions exist? What happens to the reflected wave when it reaches the source?
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There is no limit to the length of a standing wave. It only requires one reflection to get a standing wave. If there is attenuation then the standing wave will become smaller the further you go from the reflection, but there will still be some standing wave.
If the source also reflects the wave, then there will be interference between reflected waves having undergone different numbers of reflections. When attenuation is low this results in resonance, so that the amplitude of the standing wave depends on the relationship between the wavelength (frequency) and distance between the reflection and the source, as well as on the attenuation and the size of the two reflections.
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I want to make array by unit cells which I designed. now I want to feed this array. and I will use
tapered microstrip transmission line. actually I calculated the width and length of the tapered microstrip line with the formula in papers. but I don't know how to optimize the line with HFSS. because I don't know what should be value of the Zin in array input point. my means input Characteristic Impedance for Microstrip transmission is Z0 = 50 but output Impedance for tapered microstrip transmission line value should be how much?.
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I want to test RF PCBs/ Modules for defect diagnosis. Can anyone please recommend or share a comprehensive document which can help me learn procedures to test the individual active, passive RF components and the transmission lines.
P.S : I have almost all the requisite equipment like VNA, SA, Power meter etc available with me.
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Usman Shakeel you will get some help from the equipment manuals and associated support literature. You can look up different equipment vendor literature also, but be careful before applying it on your vendor test instruments, if they are instrument specific features/ properties.
You may also procure my book 'RF & μWave Measurements: For Design, Verification and Quality Control' (available from amazon in select countries) that covers theory & practice on a wide range of RF parameters.
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400kV Double circuit Transmission line with a line length of 230kM without any compensation/PIR have 390kV ZnO surge arrester on both sides. When the bus voltage of either end approaches 420kV, the charging transient causes failure of Surge arrester. In PSCAD modelling, switching over voltage of 800kVp has been noticed. While the SA is designed to withstand 650kVp for 5 cycle. What could be cause of failure of SA?
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u are welcome Mr Nizar
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Gentlemen, I am working on three PSCAD Module in the same workspace. I am using ENI transmission line data exchange and getting the following error. Could you provide me with a clue of how I can fix that error?
Attached is the error
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Hi,
I think you should assign sending and receiving signals directly to the transmission line.
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As part of my research, I need to couple a loaded, custom-sized, rectangular, waveguide (in which a hybrid mode propagates at 8.5GHz) to either a) a coaxial transmission line or b) to a standard X-band waveguide.
I need to understand the design and optimization processes for both including impedance matching and/or mode conversion as required.
What is the best, most efficient way of approaching such a task?
Any useful resources on the topic would also be very much appreciated.
Kind Regards
Simon
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ok I see ..some metamaterial..which definition for the "wave impedance" are you using.?.500 Ohm appears rather high to me and depends on the type of mode.For more detail you can consult the books by Pozar on microwave engineering
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Intermittent renewable energy sources become more efficient and reliable as the number and diversity of sources is increased. But electrical transmission over distances greater than 2000 miles may involve excessive losses. Would transmitting energy long distances by gas pipeline be more efficient?
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I want to believe over head d.c transmission supported with lines comparators will make it easier
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I am planning to build a house very close to 20 kV transmission lines. I have looked into the research and there seem to be some health concerns regarding living in proximity to power lines. However, these papers always take into consideration transmission lines of 100 kV or above. Are there any papers that take into account lover voltages, specifically 20 kV? And if you are aware of the current consensus on this topic, please share it with us.
Thank you in advance for your input.
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Is it possible to model a transmission line conductor in PSCAD software by its code-word?
code-words are turkey, sparrow, swan, sparate, etc.
If it's not possible, can anyone help me to model different conductors?
Regards,
Pouriya
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please, I canto fine TL code in pscad library can I add this code ?
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Greetings everyone. As i am trying to simulated the reported work of SPP TLs. The ultimate goal is to measure dispersion curves. But at this stage, i am unable to get the s-parameters. Actually i am confused in how to excite/radiate the transmission line. I have used different waveguide ports and discrete ports. I have designed the structure with and without SMA connectors. Please if someone can guide me about it, i can share the simulation file of CST.
Thanks in advance
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Hello,
Some related papers are attached to solve the problems.
Papers are given below.
Thanks,
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How can we simulate a microstrip transmission line in CST eigen mode solver?
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As we can see from the CST component library, there is an example of microstrip line analysis using eigenmode solver which you could check. Apparently, there are four electric boundaries from the top, bottom and two sides of the line. Two boundaries along the line are set as periodic. However, since the microstrip line radiates power to the air, but open boundaries are not allowed in this solver, you need to set up the backgrounds properties, the upper distance should be set up higher than the line which could be used to simulate the function of the air. Then you could find the modes of the line.
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Hi there,
I would be grateful if someone could let me his opinion about this question:
There is a coplanar stripline waveguide excited with a TEM mode. My question is that how to create TE and TM modes from TEM mode excitation in these waveguides?
Thank you
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Dear Sir
The generation of TE and TM mode from the TEM mode can easily be obtained by changing the angle of the feeding probe. In other words, make an inclination angle in the feeding probe in such a way that the TEM signal propagates toward one of the ground surfaces.
Good Luck
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as you know for making the phases of transmission lines symmetric we transpose the lines,i want the suitable Distancefor transposing
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The suitable distance is n(1/3) distance of line,
n : The number of transpositions across each line length.
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I need to calculate the values of R, X, G and B used in the t-model of the transmission line.
I have a 4 core wire and its data sheet, ( https://www.hesselmann.de/data-download/produktinfo/he-nycwy.pdf ).
How can I derive these values from this data?
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Hello there.
In order to compute transmission line parameters, you need a little bit more information than that. Line impedances are affected by mutual couplings between conductors, by the presence of shield wires/sheaths, line cross section, soil resistivity, system frequency etc.
If you are looking for the theoretical foundations, I would start with the paper 'Earth Return Impedances of Conductor Arrangements in Multilayer Soils—Part I: Theoretical Model' (available at Researchgate per author request). The procedure for building the impedance matrices is documented in the book Power Systems Analysis by Stevenson, I also summarized the main calculation steps in my doctoral thesis, available from my profile page.
If you just need a quick calculation based on conductor data & system information, I would try the ATP routine Line/Cable constants. The EMPT Theory Book, by Dommel, also covers the underlying theoretical concepts.
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there is only one article about measurement of step capacitance that i have mentioned to in the question. but the article is for 1944 and very old! so i need a good approach to measure the capacitance by cst.
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Model the step in CST. Move the reference plane for S11 to the step. Look at the impedance on the Smith chart. This will give you the normalised reactance or susceptance which you can easily change into capacitance, or a more complicated combination if necessary.
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Hello to all respected professionals. Hope you all are fine. I have some doubts. I am sending below.
Can you tell me the names of some useful algorithms used in net load forecasting and line loss prediction? Will the algorithms of transmission line loss prediction and electrical loss prediction be the same? Which algorithm of Machine Learning and Deep Learning has the most practical applications? Can intelligent robots be implemented without ML?
I will wait for your answers.
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This has to be studied by defining in your particular context a network of nodes.
Each node has three functionalities:
-network (link, transmit input or output, eg NN)
-data (retrieve, store, etc)
-compute (DL, ML, etc).
Once you have done this scheme, or description, everything can be clearly discussed and optimised
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The paper attached has used 39 bus system as radial distribution system but says it has transmission lines. I am confused regarding its type (transmission or distribution system). Can anyone elaborate please?
Thanks
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Its an interconnected power system contains transmission and distribution network
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A data center is supplied power from the grid as AC power, which is distributed throughout the center’s infrastructure. However, most of the electrical equipment, such as servers, solid-state disks for storage, and other IT gear within the infrastructure, (as well as the batteries storing backup power in the UPS system), require DC power. As a result, the AC power must go through multiple stages of power conversion, resulting in power losses and wasted energy. To eliminate these unnecessary conversion steps and, thereby, substantially reduce power wastage, supporters have proposed the use of high-voltage DC power distribution for these systems.
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HVDC technology has features that make it particularly attractive in some transmission applications. The number of HVDC projects committed or under study worldwide has increased in recent years, reflecting renewed interest in this proven technology in the field.
The increasing demand for green energy has forced investors in the energy industry to search for more resources at sea. Consequently, the development of energy electronics and industrial engineering has enabled offshore wind farms to be offshore and in deep water. However, its development requires, among other technologies, DC-DC conversion systems. The advantages of HVDC are given via HVAC technology with respect to transmission distance.
With the development of high-voltage valves, it was again possible to transfer DC power at high voltages and over long distances, which led to the emergence of HVDC transmission systems The guiding and basic principles on which HVDC systems are chosen in the development of the electricity system today. In the electricity industry today, due to the liberalization and increased impacts of environmental conservation, HVDC solutions are becoming more desirable for the following reasons: • Environmental advantages • Economical (cheapest solutions) • Asynchronous connections • Energy flow control • Added benefits transport (stability, energy quality etc.) ).
For more detail, you can see the following papers:
1- file:///C:/Users/dell/Downloads/energies-13-01914.pdf
( Evolution of the HVDC Link Connecting Offshore Wind Farms to Onshore Power Systems )
2- HVDC transmission overview ( DOI: 10.1109/TDC.2008.4517304)
3- High Voltage Direct Current (HVDC)Transmission Systems Technology Review Paper.
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hi, I am trying to simulate IEEE 118 bus system in matlab simulink, I have the data for transmission lines in per unit( R,X,b). the 3 phase pi section block in simulink needs zero,posiitive and negative components of R,X and C and also the line length.
these data are not available, any help /suggestion in this regard is much appreciated.
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Which software can be used for simulating IEEE 118 bus test system? Any software which has a built-in model for IEEE 118-bus?
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Basically I want to develop auto reclosing schemes in HVDC system to differentiate transient and permanent faults and automatically reclose the faulty phase of transient faults after deionization. So I need an HVDC transmission test model to test those schemes.
Thanks
Arif Mehdi
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I am looking to design/study microwave/RF heating in liquids on a CPW transmission line. The setup is slightly different from the example given in the COMSOL Application Libraries.
In my scenario, the liquid has temperature dependent relative permittivity, and a port numeric can only be used.
Anyone done this before and willing to guide my design simulations?
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This agood work and recent , zMy work parcticly not theoratical .
Ii suggest connect with theoritical studies . I hope for you a nice day
Regard
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What is the difference between different types of microstrip coupled lines show in figure attached?
What type of coupling mechanism involved in between coupled lines shown in figure attached?
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One of these is a filter. The other is a coupler. It could be a hybrid coupler.
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Firstly, thank you for being interested in my question and opening this.
I'm having a hard time calculating input impedance by transmission line theory.
I'm a student studying microwave absorbers. In this field, it is necessary to calculate input impedance to finally obtain reflection loss.
I've uploaded a file showing the equation of transmission line theory.
In the equation, I wonder how I can treat 'j' in tanh when I calculate it in excel program.
I've tried solving the tanh part in many ways like this, but I couldn't
TANH((COMPLEX(0,1))*(2*3.14*((10)^(-2))*(2/3)*((M2*N2)^(1/2))))
TANH((COMPLEX((2*3.14*((10)^(-2))*(2/3)*((N2*O2)^(1/2))),1)))
IMPRODUCT("0+1i", "(2*3.14*((10)^(-2))*(2/3)*((M2*N2)^(1/2)))+0i")
I have no idea how I should threat 'j' in tanh
I'd appreciate it if you'd help me to solve this question.
Best regards.
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Why don't you try the same using FORTRAN/C/C++/MATLAB etc numerical software. Excel is good for office work, not for research.
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The distributed amplifier is designed using lumped inductors and amplifier cells. Amplifier cells with lumped inductors constitute a lossy artificial transmission line. I can simulate and get S-parameter of the amplifier assuming its a 2-port device. I have a question regarding evaluating the propagation constant so that attenuation (real part of propagation constant) can be found.
As the length of artificial TL is not a parameter here hence I can't convert S to ABCD and find propagation constant (Gamma)
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Dear Pradeepan,
If you have sections then you can define the propagation consatnt P per section and not by unit length as in the transmission line.
For travelling wave
A( i) = Am exp ( alpha _ jbeta) i,
A is the output amplitude and Am is the input amplitude.
alpha is the attenuation or the gain constant per section and beta is the phase constant per section.
So this equation can applied on one section and on any number of sections provided they are matched.
Best wishes
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Is metamaterial same as metamaterial transmission line? Why do we need transmission line on metamaterial? Is this an antenna once we put transmission or stripline on metamaterial. Any guidance is much appreciated.
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Metamaterial transmition line is an application of metamateral
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I want to simulate a coaxial cable in FEKO software. However, the results do not agree with the transmission line solution that uses the transfer impedance (Schelkunoff model). I m thinking that the terminations in the MoM (FEKO) simulation affects the inner circuit. any suggestions.
Also, how can I extract the transfer impedance of a coaxial cable from the MoM results?
check my termination in the attached image.
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Yes, now I saw your figure. That's right . See details about "pigtail" on shielded wires: Pigtails effect on shielded wire coupling, Clayton R. Paul
1979 IEEE International Symposium on Electromagnetic Compatibility
Year: 1979 | Conference Document | Company: IEEE