Since velocity of the recorded groove is the quantity we record when we make a needle-drop (because phono cartridges are velocity sensitive devices1), it is useful to know maximum recorded velocities inscribed a gramophone record because, with this information, we may correctly calibrate preamplifier gain so as to take best advantage of the digital medium.
There is an enormous amount written about maximum recorded velocities on gramophone records: with some opinions supported with graphs and statistical measurements of various replay systems. These are useful and interesting. However measurements "after the fact" are prone to all sorts of errors and ignore physical limitations in cutting an acetate (or a metal-master) which, in any case, enforce a ceiling on recorded velocity.
In fact, there is a very simple rule. The maximum (peak) recorded velocity cannot exceed the linear, tangential groove velocity. For, if it does, the recording chisel "slews" so quickly (beyond 45°) that the chamfer on its rear edge interferes with the recorded groove.
This simple maxim is somewhat complicated in that the tangential groove-velocity changes throughout the entire volute groove. Nevertheless, we can define the limits with precision. At the outer edge of an LP record, the linear velocity is 0.509m/s (20 inches per second), and this reduces to 0.196m/s (8 inches per second) on the innermost. Thus we can say, the maximum recorded velocity on a 33⅓ RPM LP will never exceed 50cm/s, and even this figure is only achievable on the outermost groove.
This is confirmed by our own measurements of LP records which do indeed reveal that no intended modulation ever seems to exceed 50cm/s. Groove damage can produce signals above this level, but these are pathological.
We can apply this rule to other media too. Thus, a 12" 45 single can support a maximum recorded velocity of 68cm/s (although measurements frequently indicate that recorded levels on 12" singles are no greater than from LPs2). And the maximum velocity recordable in the outermost groove of a 12" 78RPM record is 118cm/s or 7.5dB greater than the maximum velocity on an LP.
The graph below relates maximum groove amplitude to recorded velocity for LPs. The standardised dimensions of an LP constrain the maximum possible groove "wiggle" to a peak amplitude (a) of 38μm (0.0015")*.
Velocity V(t) is a function of frequency f and is calculated as,
V(t) = 2 . π . f . a
If LP discs were recorded with a true constant-amplitude characteristic so that this degree of "wiggle" was maintained throughout the audio spectrum, the velocities would exceed the 50cm/s limit too early in the audio range for the medium to be viable (see the dotted section the velocity curve).
Instead, an LP recorded with a RIAA characteristic, has two regions of constant-amplitude separated by 12dB and with a falling shelf between 500Hz and 2kHz (see graph below). Maximum excursions above 2kHz are therefore limited to ¼ of the maximum peak excursion at low-frequencies, or 9.5μm (pk). This modification keeps maximum velocity below the tangential groove-speed limit until 8kHz at the edge of the disc and 3.5kHz at the end of the playing-side.
These may seem quite low frequencies and indeed they are! Gramophone records are only viable because the energy of music falls with frequency, so the medium isn't required to be able to handle full-scale modulation at all frequencies. Today we would consider it a compressed medium.
In fact, the situation is actually worse than the considerations above imply when we come to play the record, because a further limitation exists on reproduced velocity when the stylus radius dimension exceeds the radius of the recorded curve3.
Determining the miminum radius of any section of smooth curve at point (P) is part of differential geometry. The solution is known as the osculating circle (or kissing circle) which is the circle that best approximates the curvature (C) at P, as shown right.
Clearly maximum velocity can no longer be achieved once the effective radius of the stylus exceeds the radius of the osculating circle at any point in the curving path of the groove. Or, to put is more bluntly, when the stylus can no longer negotiate the corners!
We can calculate the minimum radius of (Rc) of a recorded groove4 using the formula,
Rc = v2 ÷ [ a . (2 π f )2] , where radius is in metres.
where v is tangential velocity, a is peak amplitude and f is frequency.
The results of these considerations are annotated on the main graph too (in red lines). These indicate that a "standard" 18μm (0.0007") radius stylus will fail to transduce the recorded values on the disc at all diameters of the disc surface. However, a stylus with an effective radius of 5μm (as do the best hyper-ellipticals etc.), will keep ahead of the limitations due to cutting at all recorded radii.
No better argument could be advanced for the superiority of hyper-elliptical stylus and its cousins such as the Shibata, although it should be bourne in mind that a cartridge fitted with a stylus of this type have the capacity to produce peak electrical levels over twice that of the conical type for the same nominal sensitivity.
1. Even a crystal (ceramic) cartridge outputs a measure of the groove velocity if it is appropriately loaded as explained here.
2. We suspect the reason for this is that the cutting-engineer is working with a single track and has no scope gradually to reduce recorded-level throughout the duration of the side which is a standard trick with LPs. She is therefore constrained to work within the inner groove velocity-limit; which is 27cm/s on a 45 RPM 12" single.
3. It is also possible to think of this as an acceleration limit. Thus velocity limits exist when cutting a record and acceleration limits exist in reproduction. Naturally the moments of highest acceleration coincide with the points of greatest curvature. Actually, this is something of a simplification because acceleration is sometimes, and deliberately, limited during cutting too.
4. The reciprocal of this value is called maximum curvature: a big number expressing a small radius.
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