Ivar KJELBERG
COMSOL Multiphysics(r) fan, retired, former "Senior Expert" at CSEM SA (CH)
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Posted:
1 decade ago
Sep 19, 2012, 3:06 a.m. EDT
Hi
indeed V4.3 has changed something, I believe it was different in 4.2, this needs some more testing ;)
--
Good luck
Ivar
Hi
indeed V4.3 has changed something, I believe it was different in 4.2, this needs some more testing ;)
--
Good luck
Ivar
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Posted:
1 decade ago
Sep 19, 2012, 11:03 a.m. EDT
Hello,
I have the same problem (version 4.2), as I described here
www.comsol.com/community/forums/general/thread/12098/
The pzt beam behaves like a voltage generator: changing the impedance of the circuit, only the current changes.
Indeed the piezo beam should be affected by the electric load and vice versa.
Hello,
I have the same problem (version 4.2), as I described here http://www.comsol.com/community/forums/general/thread/12098/
The pzt beam behaves like a voltage generator: changing the impedance of the circuit, only the current changes.
Indeed the piezo beam should be affected by the electric load and vice versa.
Ivar KJELBERG
COMSOL Multiphysics(r) fan, retired, former "Senior Expert" at CSEM SA (CH)
Please login with a confirmed email address before reporting spam
Posted:
1 decade ago
Sep 21, 2012, 7:43 a.m. EDT
Hello again,
How many elements do you have in the thickness of your PZT ? to see any effect on the damping versus CIR impedance you need at least 5 if possible far more in the THICKNESS (between the electrodes ;)
Or is it all "just" a mesh density effect, I would like to see the "k" factor come out
By the way CIR does not seem to be set up form eigenfrequency mode analysis (?)
--
Good luck
Ivar
Hello again,
How many elements do you have in the thickness of your PZT ? to see any effect on the damping versus CIR impedance you need at least 5 if possible far more in the THICKNESS (between the electrodes ;)
Or is it all "just" a mesh density effect, I would like to see the "k" factor come out
By the way CIR does not seem to be set up form eigenfrequency mode analysis (?)
--
Good luck
Ivar
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Posted:
1 decade ago
Sep 23, 2012, 5:21 a.m. EDT
Hello Ivar,
I have attached my model. I have 6 elements between the electrodes, but I still can not see any dependence of the electrical impedance in the CIR.
I would expect that the output power is dependent on the electrical load, but varying the resistance there is no change in the mechanical or electrical behavior of the beam.
Maybe I have set wrong conditions (the "terminated" Terminal could help?), or maybe wrong analysis (indeed you cannot use eigenfreq analysis with CIR physics).
Thanks in advance
Hello Ivar,
I have attached my model. I have 6 elements between the electrodes, but I still can not see any dependence of the electrical impedance in the CIR.
I would expect that the output power is dependent on the electrical load, but varying the resistance there is no change in the mechanical or electrical behavior of the beam.
Maybe I have set wrong conditions (the "terminated" Terminal could help?), or maybe wrong analysis (indeed you cannot use eigenfreq analysis with CIR physics).
Thanks in advance
Ivar KJELBERG
COMSOL Multiphysics(r) fan, retired, former "Senior Expert" at CSEM SA (CH)
Please login with a confirmed email address before reporting spam
Posted:
1 decade ago
Sep 24, 2012, 1:48 a.m. EDT
Hi
Indeed something seems to have changed over the last versions.
First of all with CIR I do not get any differences either, even if I see a difference in the induced voltage along the thickness of the beam (when you have more than 3 elements in the thickness ;)
So there are two comments / warnings for CIR "External I Terminal", as well as the one I usually use "External I vs U Terminal" about back coupling the current source, this might need something more.
But anyhow in stationary, at time t= INF the current is = 0
So I believe one need transient or harmonic /frequency sweep cases.
Anyhow, you can also use the terminal node alone without CIR physics, by adapting power input and changing manually the impedance from 1 to 1E6 ohm
So try to add a frequency domain solver at 20 Hz, remove (delete fully) the CIR physics, first disable the floating terminal, then set the terminal 1 to Terminated, 0 mW and User defined impedance 1 Ohm, then derived variables average line 8, dump the values of u2 and v2 into a table. Change the impedance to 1E6 ohm and run again, check the average u2, v2, then enable floating terminal and run again, you will see the displacement amplitudes at 50 Hz are slightly different, with a damping (imaginary part) when you change R, but no damping with the Floating terminal
Now you can try to change the mesh density and see the effects
And CIR seems not to accept eigenfrequency PZD solutions, again looks like some (back)coupling is missing that we have to set up manually, this needs more thoughts, even Multiphysics require that we fully understands what is behind it all ...
--
Good luck
Ivar
Hi
Indeed something seems to have changed over the last versions.
First of all with CIR I do not get any differences either, even if I see a difference in the induced voltage along the thickness of the beam (when you have more than 3 elements in the thickness ;)
So there are two comments / warnings for CIR "External I Terminal", as well as the one I usually use "External I vs U Terminal" about back coupling the current source, this might need something more.
But anyhow in stationary, at time t= INF the current is = 0
So I believe one need transient or harmonic /frequency sweep cases.
Anyhow, you can also use the terminal node alone without CIR physics, by adapting power input and changing manually the impedance from 1 to 1E6 ohm
So try to add a frequency domain solver at 20 Hz, remove (delete fully) the CIR physics, first disable the floating terminal, then set the terminal 1 to Terminated, 0 mW and User defined impedance 1 Ohm, then derived variables average line 8, dump the values of u2 and v2 into a table. Change the impedance to 1E6 ohm and run again, check the average u2, v2, then enable floating terminal and run again, you will see the displacement amplitudes at 50 Hz are slightly different, with a damping (imaginary part) when you change R, but no damping with the Floating terminal
Now you can try to change the mesh density and see the effects
And CIR seems not to accept eigenfrequency PZD solutions, again looks like some (back)coupling is missing that we have to set up manually, this needs more thoughts, even Multiphysics require that we fully understands what is behind it all ...
--
Good luck
Ivar
Please login with a confirmed email address before reporting spam
Posted:
1 decade ago
Oct 8, 2012, 7:10 p.m. EDT
Hi Ivar,
Thank you very much for your help.
I tried to follow your suggestions, but I have noticed 2 things:
- during the eigenfrequency analysis, changing the resistance value, the natural frequency has a very small variation; instead if I use a frequency domain analysis, the resistance is very effective on the natural frequency.
- using this frequency domain analysis on the resistance I get a complex voltage value. I suppose that it is a phasor, whose phase refers to the applied load. But the current, although there is a resistive load, does not have the same phase.
Another thing: what is the difference between eigenfrequency and eigenvalue analysis? does the eigenfrequency consider the damping matrix?
Thanks
Damiano
Hi Ivar,
Thank you very much for your help.
I tried to follow your suggestions, but I have noticed 2 things:
- during the eigenfrequency analysis, changing the resistance value, the natural frequency has a very small variation; instead if I use a frequency domain analysis, the resistance is very effective on the natural frequency.
- using this frequency domain analysis on the resistance I get a complex voltage value. I suppose that it is a phasor, whose phase refers to the applied load. But the current, although there is a resistive load, does not have the same phase.
Another thing: what is the difference between eigenfrequency and eigenvalue analysis? does the eigenfrequency consider the damping matrix?
Thanks
Damiano