Orb, I am no expert in LP technology
. That said, I did read through Paul's segment:
http://www.zinio.com/reader.jsp?issue=416125359&o=int&prev=si&p=92
My read is that he is talking about a secondary effect. The primary is what was stated before: which is the resonance caused by the *spring* in the cartridge combined with the mass of the tonearm. As Tom mentioned, these are in 0 to 20 Hz.
What Paul is appearing to talk about is that the tonearm itself flexes. And therefore, it creates another set of modes that are the frequencies mentioned. You can see this in the way he explains this effect with respect to the loading that the cartridge puts on the tonearm as simple weight as opposed to spring above. Since the tonearm is much stiffer than the cartridge spring, it reasons that it would have higher resonance frequency.
Take another look with this context and let me know if you disagree.
I understand that, but it is a combination of 1st,2nd,3rd modes and how this interracts can only truly be seen by looking at the cumalitve resonant decay spectrum that relies upon the mechanical input.
As an example the Linn Akito has 2 clear resonant modes that are visible in the Jun 2010 group test.
Two clear resonant modes are visible on the cumulative decay plot, the main armtube bending at 230hz and 1.2khz, with another series at 800hz showing harmonics at 1,6khz 2.4 and 3.2khz.
Importantly these modes are very well damped, falling by 40db over the 40msec window.
The point is while I only partially quoted the opinion previously, it is these that affect the sound generated by tonearm resonances, including arm break, and why he measures these as part of the cumulative resonant decay spectrum, importantly these are affected by the cartridge
If you look at cartrige measurements the "spring" does not come into this in way discussed, specifically he focuses more on the L-R and L+R on what affects the sound, which I touched upon earlier in the demag thread.
BTW I am definitely no expert as well
but I have all the investigation articles and the other articles by Paul Miller, along with comments and measurements for individual and group tests.
Just so we do not get crossed wires on semantics Paul in the article I think your talking about also says this:
If the arm moves relative to the stylus then the recovered audio is modulated adding "color", musical or otherwise.
The cumulative resonant decay plots that accompany our reviews illustrate this.....
So for a true accurate picture of resonance effect, we must consider the tonearm with cartridge included and cannot think of its own trait, still the resonant affect on sound comes back primarily to the tonearm.
However I am yet to see Paul Miller mention any type of cartridge resonance in his discussions or measurements (even for cartridges) but I appreciate I may had missed them.
The closest I see to this is the following but then the main operation seems to be vibration linking to tonearm:
All seasoned vinyl fans understand the need to match cartridge compliance to the arm's effective mass to avoid resonance with warped LPs, at the other extreme, subsonic groove detail...
In truth , the little beggars bend,ripple,twist and even expand and contract in response to noise (vibrations) from the body of the cartridge.
I do appreciate we may be crossing semantics and different focus on where the primary resonance (or alternatively it is vibration noise instead) originates from or should be the focus-affecting the sound.
Where he does say:
The natural frequency of the arm is proportional to its mass and stiffness but is readily "tuned" by your choice of cartridge and compliance of its mounting to the deck.
But for his parameters relating to cartridges and their impact on sound or performance (March 2011), resonance is not one of them.
Cheers
Orb