Trombone instructors ask their students to strive to play with constant air flow through the instrument. Some instructors advise practicing by lip-buzzing into a mouthpiece connected to a disposable medical spirometer. The acoustic impedance of such a kludge is vastly different from that of a trombone, so the feel of playing a trombone is lost. I describe here a device that monitors air flow into a trombone while it is being played.
Every trombone mouthpiece consists of a large cup followed by a focal narrowing (throat) followed by a bore (backbore) of larger diameter than the throat. This construction lends itself to use in a Venturi flowmeter, in which pressure-sampling orifices are placed in the cup and throat. The pressure differential between the two orifices is an indicator of flow. I drilled into the cup and backbore close to the throat of an old sacrificial mouthpiece (and later a new one) and cemented stainless steel tubes into the drilled holes. A cemented baffle made from a bisected plumbing washer provides a barrier between the sampling orifice in the cup and the direct air jet entering the cup.* Flexible plastic tubing leads away from the mouthpiece to a display unit. I used tubing from medical IV sets.
Initially I measured pressure differences with a differential transducer followed by a D.C. amplifier. This approach failed because a large-amplitude alternating pressure component superimposed on a much smaller average level evidently swamped the differential transducer. The transducer output, even with lowpass filtering, did not reliably reflect air flow. I achieved improvement with acoustic filtering of the mouthpiece signals by inserting a tiny pinhole within each sampling tube at the mouthpiece. These resistive series elements in conjunction with the air volume in the plastic tubing formed lowpass filtering that effectively removed the alternating pressure component proximal to the transducer. Then all was well until the tiny orifices became obstructed with fluid, which they did frequently, requiring clearing with compressed air. However, the concept was proved.
The key to a successful design was the use of two gauge-type transducers, one for each sampling orifice, each followed by electronic lowpass filtering, the two signals then compared in a differential amplifier. The tiny resistive orifices were eliminated, so the air pathways from mouthpiece to transducers were wide open.
The 100K resistors at the transducer outputs followed by 1uf capacitors to ground provide the lowpass filtering. The signals then go to a differential amplifier which drives a variable gain amplifier to set sensitivity; this stage drives the bargraph. The transducers are NXP model MPXV7007, specified to measure -1 to 1 psi, corresponding to 0.5 to 4.5V output. The LED display is a Barmeter Electronics model AE151S29Z 05CA7021H. The odd power supply potentials are due to tailoring to parts on hand.
In the oscilloscope photo Ch1 & Ch2 are filtered and unfiltered backbore signals; Ch3 & Ch4 are filtered and unfiltered cup signals. The center line is zero volts. Note the difference in sensitivities between the filtered and unfiltered traces -- the p-p unfiltered signal voltages are more than an order of magnitude greater than the filtered averages. Instantaneous pressures go well below atmospheric. The note played was a middle Bb (about 233Hz) at moderate volume.
*Purists may point out that the baffle affects acoustic impedance and therefore the playing characteristics of the mouthpiece and trombone. This is true, but the effect is not great -- about the same as experienced between unmodified standard mouthpieces having different specifications.