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.
Positioning the Optical Sensor
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 |
Unblocked and blocked voltages for different fork gaps
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.