Back guide of the clavichord key levers
Key levers of the clavichords are required to be noise free and less sensitive
to environmental changes, such as humidity and temperature. Vast majority
of the historically made clavichords have so called rack/tongue mechanisms,
which use small piece of wood, metal or bone, sliding in slots cut on a
diapason rail underneath the hitch pin rail. It is extremely difficult
to reduce the noise below the acceptable leve, due to the friction between the tongue and the slot. From the noise
stand point, C. G. Hubert's silent action is superior. However, as two
pins at the both sides support the back end of the key levers, it has a
disadvantage to be directly affected from the environmental change.
The guide shown on the left is developed from both low noise level and
low sensitivity to the environmental changes. The metal pin does not contact
to the wood, but only with the leather attached on the top and bottom of
the key lever. Any changes of the key lever width, due to the environmental
changes, do not directly affect to the width of the slot cut on the leather.
At the higher notes, key lever width may not be enough to put the pin on
its center. In this case, the leather pieces on the top and the bottom
are attached overhanging from the key lever width and pins at the both
sides support the key lever. Environmental changes of the key lever width
are always below the acceptable level as any changes is proportional to
the small key width.
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Put a bending fixture on an outdoor camping stove, then one end of the
bentside board is clamped on the fixture and the other end is pulled down
to give a proper curvature. To bend the board for a large area, the clamping
position can be repeatedly moved as needed. Bending compliance of the board
cannot be homogeneous and the board can be slightly twisted after removing
the force and the temperature. If it happened, the pulling force at the
both sides of the board can be independently adjusted. Using an industrial
heat-gun, locally applying additional heat is sometimes effective for correcting
the twist. Careful management of temperature is necessary not to burn the
board.
The photo on the left is showing the bending process for a double bentside
of a Germann harpsichord.
When a higher wire tension is required, either longer speaking length,
thicker wire or heavier materials can be employed. Brass strings, having
heavier specific gravity than iron, need to be stretched with higher tension
to achieve the same pitch. If materials heavier than brass is used, instruments
can have strings with even higher tension. However, from the practical
point of view , no materials other than brass or other copper alloy can
be found. It is difficult to have harmonics rich sound with too thick strings.
Then, an over-spun wire, is used. It provides heavier effective density
by winding a soft and heavy wire over the core string.
String tension can be calculated with pitch(frequency), speaking length
and weight per unit length of the wire. The weight per unit length is calculated
with diameter and bulk density of the wire. It is convenient to use an
effective weight per unit length calculated with an apparent bulk density
of the over-spun wire. The formula to give the apparent density can be
found here.
Detailed description of the winding machine can be seen by clicking below
photos.

A hand drill is used as a power source. The lever in the front is a power
switch. Two individual gear boxes, located at right and left ends, are
connected with a hexagonal bar.

The left gear box, connected with a hexagonal bar, is fixed on a workbench
with a clamp. The left gear box can be clamped at any position according
to the wire length. The clamp is also convenient to apply tension to the
core wire.
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A magnetic device to measure sound board thickness
@Assuming a detailed explanations of how the device works is not widely available, though sometimes it is referred as "magnetic method", a schematic drawing, showing the principle of the measurement, is provided below. Measurement accuracy is not as good as those with dial gauges. However, the accuracy can be statistically improved by measuring several times and average them.
The schematic drawing shows only the principle. The blue arm in the left is slowly pulled-up. As soon as the magnet, attached to he coil spring, separates from the board, read the thickness of the board, indicated on the scale (red colored). Another magnet below the board still stays there. The blue arm needs to be pulled more, if the board is thinner.
When the outer case, which has a scale, is pulled up, the coil spring is streched and upword force is applied to the magnet, above the soundboard material. When the upword force becomes greater than the magnetic attraction force with another magnet under the board, the upper magnet comes apart from the board. At this moment, the scale indicate the thickness of the board.
Wire tension can be calculated with following formulas.
,
, 
where:
T: Tension
L: Speaking length
d: Diameter of the wire
f: Resonance frequency
r: Bulk density of the wire material
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Apparent density of wound wire can be calculated, using below formula:
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where:
ra: apparent bulk density for tensile load
rc: bulk density of the core wire material
rw: bulk density of the cover wire material
dc: diameter of the core wire
dw: diameter of the cover wire
N: number of turns per unit length
By pressing below buttons, calculated results of string tension for each
of the instruments shown in this web site are available.
German Harpsichord 8feet German
Harpsichord 4 feet
Italian Harpsichord
Italian Virginal
French Harpsichord 8 feet
Flemish Harpsichord 8feet Flemish Harpsichord 4
feet
Flemish
Virginal
Square
Piano
Fretted Clavichord Unfretted Clavichord
Geigenwerk Geigenwerk2 Streichklavier