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The force numbers they use in this report are misleading at best. Actually close to fraudulent. The forces they give are based upon static friction due to static weight. .7gram per side(each groove wall) from a static load of 1.4gr of tracking force. That number is correct, except the groove does not see static forces during play. Kenetic friction is always lower than static friction. The kenetic friction forces will vary depending upon frequency.Low frequency = higher kenetic friction, yet still lower than static. High frequncy = lower kenetic friction.A phenomena occurs when friction goes from static to kenetic called moment of motion This is not moment of inertia. During that "moment" from static to kenetic, energy drops 90deg in relation to the static (fiction) vector.
Marc, have you been drinking again? J/K
From Handbook for Sound Engineers [ The vertical tracking force applied to the stylus is divided between the two walls. Each wall is experiencing force that is equal to the total vertical force times the cosine of 45 degrees or .707(Fig. 23-117) For instance if the vertical tracking force (VTF) is 1g,then each groove wall will experience a force of .7g. This wedge effect plays an important role in understanding the dynamic behavior of of the stylus in a compliant groove and its effect on electrical separation between the channels.]I run an AT 440ML and I use a VTF of 1.4 grams which when multiplied times .707 yields a .9898 gram force on the groove walls. This is 30% higher than the above cited example. Many moving coils track at 1.8g. to 2.2g. VTF. In the case of the 2.2g. VTF this would yield a force on each groove wall of 1.5554g. which is more than double the force of a 1 gram VTF.If anything the 1VTF in the example was overly conservative and was obviously chosen for how neatly the math works out. In the real world the forces on the groove wall can easily be more than twice as high. The key point here is that the forces exerted on the groove walls are sufficient to generate temperatures above the melting point of vinyl which is 480 degrees F.. The micro-melting at the point where the stylus contacts the groove wall is also a critical factor in reducing record wear. When a coolant is used on the surface of the vinyl record and melting is inhibited the stylus starts to behave like a cutting tool on lathe instead of device for recovering information on a record. Scotty
BaMorin, is it your contention via this argument that it is okay to play your records wet? Apparently there is an adequate amount of "Factor X" to cause melting at the point of contact under the dynamic conditions that exist during playback. I strongly suspect that the reason that the scope of the treatment of this subject in the Sams book was limited to static conditions only is because an in depth analysis of the factors in play under dynamic conditions is not practical or possible. For example imagine the increase in force against the groove walls due to instantaneous G loading as a result of the lateral accelerations encountered while tracing the undulating groove.Scotty
It would interesting to attempt to measure the temperature with an non-contact infrared thermometer. The melting would be easy too see with modern video techniques the temperature may be much more difficult to measure because the contact area is under the diamond. Given that the vinyl almost immediately re-freezes and is therefore less than the melting point on the trailing side of the diamond I wouldn't be surprised at some experimental error creeping into the temperature measurement.Scotty
simple experiment.........take a piece of a broken record, melt it and then see how long it takes to get hard again. I ain't buying it immediatly re-freezes. I ain't buying it melts in the first place. The photos show impact damage. The pseudo-science claims melting due to friction, yet no friction numbers are given. Only load factors. I can run a car into a tree to show load factor damage......friction wouldn't have a thing to do with it.