(Photograph courtesy of Art Reblitz)
Mills Novelty Company early piano
relay/resister expression system electrical schematic. In the
above schematic, the music roll feeder assembly is represented
by the circular drums at the drawing's right side, with the
contact roller shown as grounded. Thus, when a music roll
perforation moves over the grounded contact roller a tiny wire
brush makes an electrical contact, thus actuating some
particular function.
The "upper bus" piano magnet coil shown
(near the center top of the schematic) is representative of ALL
the piano magnets included in that electrical bus. The same
analogy is true for the so-called "lower bus," the two buses
then essentially dividing in half the electrical load for
operating the piano note scale. When a brush connected to a
piano magnet, in either the "upper" or "lower" bus, makes
contact the corresponding piano note plays at a moderate or
"medium" intensity.
The "M" at the upper left of the drawing is
the positive voltage feed, whereas the feeder contact roller is
the ground return for any electrical circuit. Because of the
dropping resister, represented by R1, R2, R3, and R4, the
voltage to piano magnets is reduced, mainly by R1 for the
"upper" bus, and by R4 for the "lower" bus. This voltage drop
causes the piano notes to play at a moderate intensity. This is
the default state of the piano expression system.
When
the "loud" relay is energized (by music roll perforation #120)
the dropping resister is effectively removed from the circuit,
and so any piano note energized operates at full voltage, and
therefore plays at full or loud intensity. For soft notes, music
roll perforation #122 grounds the center tap of the resistor
network. This causes increased current flow through resistor
segments R1 and R4, which results in a further and significant
voltage drop, thereby causing any piano magnets energized to
play at low or soft volume. The amount of additional voltage
drop for the soft setting is determined by the value of
resistors R2 and R3. The lower the resistance of R2 and R3 the
greater the current flow and subsequent voltage drop across
resistors R1 and R4, and conversely the greater the resistance
of R2 and R3 the less the voltage drop.
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