helical coil operating at 13.56MHz boundary conditions in hfss
I have designed a single turn coil radius=10cm and thickness 5mm, I need to find the resonance frequency of the coil using hfss
the theoretical calculated inductance is .464 uH and for the coil to resonate at 13.56 MHz approximately i need to add a lumped capacitance of value 330pF.
I tried to assign radiation boundaries at more than lambda/4 distance dat is 530cm from the coil and applied a lumped cap value of 330pF but it shows the s-parameter curve at nearly 500MHz range
and surprisingly whn i changed the value of capacitance there is no effect on the result.
could anyone tell y the lumpedcap is not effecting the resonance of the structure and also assigning the right boundary conditions.
could anyone help me to solve this problem...
the radiation boundary is not shown in the figure given below..
if anyone needs the hfss file i could upload that too for your convince to go through my problem
To get resonance near 500 MHz using a 330pF capacitor, the inductor should be about 0.4nH (400pH).
So, I assume your inductance calculation is wrong.
I mentioned that i designed for 13.56MHz but i am getting the simulation result around 500Mhz and the simulation shows no variation if i change the capacitance also.
Your calculation is right.
I used to design a coil like you and have the almost same results. In my case,radiation boundary is 2.5 meter from coil.
Your lumped capacitor is strange and different from mine.
Can you upload your HFSS file and I will check?
Thuan
Pls check the attached file
Getting it to resonate, and making it an efficient antenna are two very different goals.
Just connecting 330pF would make for a very low overall impedance, in which the resonant Q would also be extremely low.
Not only that, the radiation of both E and H fields will be extremely inefficient because the physical dimensions are very small with respect to the wavelength.
For effective radiation or absorption, you need two things.
A reasonably high operating Q at resonance, where the resonant amplitude builds up.
And physical dimensions that can launch an effective amount of energy into free space.
The physical size of your ring are much more appropriate for the wavelength at 500 Mhz, where one complete wavelength is about 0.6 metres, or very close to the circumference of your ring.
At 13.56 Mhz, one complete wavelength is about 22 metres.
Put simply, such a small physical device is not going to either generate, or capture 22 metre long waves very efficiently.
Thank you for your kind reply,
But I was trying to design the antenna based on a paper published in Progress In Electromagnetics Research, Vol. 138, 197-209, 2013 : LOOP SWITCHING TECHNIQUE FOR WIRELESS POWER TRANSFER USING MAGNETIC RESONANCE COUPLING.
Pls go through the attached image of the table presented in the article regarding the obtained values.
Kindly provide me with your suggestions
Magnetic resonance coupling is an entirely different principle to the electromagnetic generation of radio waves.
What you are trying to do has more in common with a (tuned) electrical transformer.
The electric or E field is not relevant here.
The H or magnetic field becomes of of vital importance, because that is all there is.
To generate a strong magnetic field you need to enclose as large an area as possible with as many ampere turns as possible. And resonance is a very efficient way of multiplying the current for any given input power level.
A single turn will certainly work, but multi turns will work a lot better if at all physically possible.
Its a case of driving enough current through what you have at the transmitting side.
Is there any reason why you cannot enclose several turns into a single loop instead of just having one single turn ?
It dramatically raises the impedance and much higher circuit Q is possible.
It will raise efficiency at both transmitting and receiving ends.
Loop antennas are nothing new, they have been used for over a hundred years for radio direction finding at low to mid radio frequencies.
http://en.wikipedia.org/wiki/Loop_antenna
Thanks for the clarification.
What I am designing here is a 4 coil wireless power transmission system, the source and load coils are single turns and Tx and Rx coils are multi-turn coils as you said, I have to design the system such that it resonates at 13.56 MHz. for the optimization i have to built each coil such that it resonates at 13.56 MHz. but when I design the single turn itself, it shows the result above 500 MHz.
Could you please provide the suggestions regarding boundary, it it the H boundary that I have to specify while simulation or the E boundary?
Thank you.
I'm not using HFSS, but according to empirical inductor formulas, the shown design (10 cm loop, 330 pF) should resonate in the 10 MHz range, I think rather 17 than 13.6 MHz. There will be also a high frequency resonance of the shorted ring.
The fact that you don't see the low frequency resonance suggests that your setup is somehow unsuitable. As Warpspeed already mentioned, the inductive transmitter coil can be simulated as pure AC electromagnetical problem, without considering the E-field or the coupling to farfield. But in this case you only get the loop inductance and ESR.
How do you observe resonance?
You will not be able to efficiently resonate the coil all by itself, except at 500 Mhz which is its own natural frequency, and requires no resonating capacitors to achieve that.
The further you try to pull it down in frequency by adding capacitors, just destroys the Q to the point that any resonance peaking effect will be difficult to measure.
So another different approach is needed.
The way a normal radio transmitter works is you have a tuned tank circuit within the transmitter, and then you couple that into the antenna. The antenna itself may or may not be resonant, but with the correct degree of coupling the antenna becomes an extension of the tuned circuit within the transmitter.
If the coupling is too loose, insufficient energy reaches the antenna.
If coupling is made too tight, the non resonant antenna damps out the resonance of the tuned circuit in the transmitter, and killing the free amplitude buildup that resonance provides..
When tuning a radio transmitter, there are two controls, "tuning" and "loading".
Both need to set optimally for maximum output into the antenna.
What I think you may need here is something similar. Your power source at 13.56 Mhz needs to resonate a pretty efficient tuned circuit, where resonant energy is allowed to build up to a significant level.
You then couple your radiating loop to that, such that you can get maximum current circulating around that loop at 13.56 Mhz.
The loop itself will not be resonant, but it draws resonant energy away from the actual correctly tuned resonant part, but not so much that it kills the resonant peak.
Generally transmitter tuned tank circuits are arranged to have a loaded Q of about seven to ten (typically). You need to adjust the coupling of your loop to achieve those sorts of values.
Thank you for the reply.
But. most of the papers or articles indicates they tune each coil in the 4 coil wireless power transfer system to have a self resonance frequency in here it is 13.56 MHz, What you have mentioned about the entire system is correct abt tuning by adjusting the coupling.
for me in the current work I could not tune each coil to the self resonance frequency. Please find the attached file whr they indicated the self resonance frequency. This is only one of the paper i am referring to for my work.
You can simulate the EM problem (inductor or coupled inductors) separately, without capacitor. The capacitor for resonance can be included later at circuit simulation level, and does not change the EM part. This separate simulation is the standard method for this type of work.