Figure 1 shows how the different components of the monochord fit
together. The longitudinal supports
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Summary: This module describes assembly of the RealSimple monochord. The monochord consists of a steel guitar string, rigidly terminated and stretched to a variable tension. Both optical and magnetic pickups are used. Subsequent laboratory exercises are concerned with making elementary measurements and observations of monochord vibration and decay.
Figure 1 shows how the different components of the monochord fit
together. The longitudinal supports
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Optional optical sensors (typically less than $10 each–in the US, see Mouser Electronicshttp://www.mouser.com/):
Neodymium magnet suppliers:
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For a horizontal magnetic field, the Magnet Holder is held vertically by two small clamps (see photographs). It can easily be moved along the string, and can also be rotated 90 degrees for a vertical magnetic field.
The signal levels are low. Using a 9V battery supply reduces possible problems with hum and earth (ground) loops. The output signal is proportional to the string velocity.
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Each transducer is a LED/phototransistor pair that are mounted facing each other, in what is henceforth called a "fork." The fork must be carefully positioned such that the string at rest partially obstructs the light passing from LED to the phototransistor. The string does not need to be an electrical conductor. Optical transducers measure the string's displacement. With two of them mounted at right angles, both horizontal and vertical deflection can be measured. Optical transducers are best mounted near one end of the string.
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The optical transducer can be correctly positioned using only a voltmeter, measuring the output voltage of the circuit shown above.
Test the fork by measuring the output voltage both for unobstructed light and when the light is blocked by an opaque object. This will give the working range. An example is shown in the table.
Note that stray light in the room should not significantly affect the result, due to the filter on the phototransistor that passes only infrared light.
| Fork gap | Unblocked [V] | Blocked [V] |
| 9.5 mm | 5.63 | 3.15 |
| 6 mm | 5.3 | 3.0 |
| 3 mm | 5.3 | 2.9 |
Select the resting point as the voltage midpoint between the two extremes. Adjust the position of the fork so that the midpoint voltage is reached. Start from the unobstructed position and move the fork slowly.
For example, with a violin G string of .75 mm diameter, we might have: Fork gap 9.5 mm, unblocked 4.8 V, blocked 3.4 V, giving a midpoint voltage of 4.1 V.
The position must be accurate to a few tenths of a millimeter. When acquiring the string vibrations, the oscilloscope and/or sound card should be AC-coupled. Sound cards are almost always AC-coupled.
The optical method requires 10 times higher accuracy for positioning than does the magnetic method. The magnetic velocity signal can be time-integrated to give displacement, which is physically more intuitive.
Figure 8 shows how the power supply connections for the optical and magnetic sensor components should be connected together. The sentinel LED indicates whether the circuits are on or off to help avoid inadvertently draining the battery.
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