| | Shop | | Payment/Shipping | | Contact | | About | | Images | | Links | | Reviews | |
A glance into the Whistlemaker's Notebook
|
Length to bore ratioShaft wall thicknessThe mouthpiece windowVertical lip positionWindway heightTunabilityChamfered windway-exitWindway shapeConical (tapered) boresThe cavity underneath the windwayUndercutting of fingerholesThe cavity underneath the windway, tapered bores and octave tuningDifferent materialsPurpose or circumstanceIntroduction:
This document is by no means the last and final word on the topic of whistle-design.
|
|
A low cut-up reduces the breathing pressure required to produce a certain volume of sound, and also tends to make the sound less breathy.
|
|
The lip's vertical position relative to the window exit is the most critical parameter when designing a whistle.
|
|
If anyone wants to learn the secrets of whistle mouthpieces, purchase a bunch of cheap whistles and split the mouthpieces as shown in the drawing above.
|
|
The windway height is perhaps not so critical as the lip's vertical position,
|
What determines the lowest note of a whistle is the distance between the center of the mouthpiece window and the end of the shaft.
Now, the fingerholes are located in accordance to this length so that the
whistle plays the scale correctly.
|
|
All of the above methods will introduce abrupt changes in the internal bore that will create turbulence in addition to messing up the scale.
|
|
In the image above you can see a trick used when making recorder-flutes.
|
|
When the windway area is greater at the inlet than at the exit, it makes the sound go loud.
|
|
"A" shows the easiest way, where the block is simply made from some piece of rod I have come up with some theories based on observation, experience and some testing, but I fear that whistle-physics is a bit more complex than what it seems to be. From what I can hear when playing different whistles, a straight bore has some problems with the second octave being too low in pitch. A conical bore on the other hand, has a problem with the second octave having too high a pitch. My only experience with tapered bores are the Clarke original and the Clarke Sweetone. The Clarke original in particular have a second octave which is very high pitched. Problematically high in fact. To get the second octave in tune you need to blow with very little strength, which makes you loose a decent tone quality completely. By looking at the Clarke whistles, it is noted that the diameter at the mouthpiece-end is quite large, while at the bell-end it is quite small. -A quite extreme taper so it seems. One could express the taper in terms of length to bore ratios. One L/B-ratio at the mouthpiece-end, and another L/B-ratio at the bell-end. The L/B ratios for the Clarke original are: 1:16 to 1:30. To me it seems that the more extreme taper, the higher the second octave will be in pitch. Is there some rule of thumb for an optimum degree of taper? I've been studying the measurment-ratios using a photo of the Copeland low-D whistles. It turnes out that the bell-end of these whistles has a diameter which is 70% of the diameter found at the mouthpiece-end. This might be a crude rule of thumb, and since the Copeland whistles sound very good, I guess this would be a rule of thumb as good as any as far as taper degree is concerned. As mentioned before, straight bored whistles suffer from a second octave being slightly low pitched. This, however has never been experienced as a problem, at least not for me. The problem arises when the Clarke manufacturer and others try to solve the second octave problem by making, in my opinion, an extreme degree of taper, since now the pitch of the second octave becomes way to high. It would be like drowning someone who's hair is on fire. That's equal to solving a small problem by introducing a more serious one. I wish I knew more about physics, since then it would be easier to understand the "mechanics" of these things. However, I do have an idea about what's going on inside the mysteries of tapered bores and octave tuning etc. 1) The clarinet for instance, has a straight bore and a reed inserted at one end. When a reed is inserted like this, it is said that the clarinet is a closed resonance tube. 2) The whistle and the flute has no reeds, but a sound-hole, and is said to be open resonance tubes. 3) For a straight bore, the closed resonance arrangement (a reed instead of a sound-hole) causes the second octave notes to jump up one and a half octave (clarinet). The open resonance arrangement (whistles/flutes) causes the octave to jump one octave only. 4) We know that a small sound-hole or a small mouthpiece window causes the second octave to go sharp, while a large sound-hole or a large mouthpiece window causes the second octave to go flat. I can't see any other reason for this that as the soundhole/mouthpiece window is made smaller, it gets more and more equal to a closed resonance system, consequently causing the raise in second octave pitch. The chanter of the Uilleann-Pipes has an octave relationship like that of flute and whistles, despite the fact that the Uilleann-Pipe chanter is a closed resonance system. -Why??? -Because it has a taper that widens towards the bell-end, a shape that evidently lowers the pitch of the second octave notes. Is this why flutes and whistles that have an opposite taper (smaller as you approach the bell-end) tends to go higher in pitch on the second octave notes? The practical consequence of this would be that a bore-diameter that gets smaller as you approach the bell-end will raise second octave pitch, and more so if the degree of this taper is extreme. (Is this the explanation why the Clarke Original has a lower pitched second octave compared to the Clarke Sweetone? The Clarke Original does have a much larger mouthpiece window). In opposition, as the taper gets wider towards the bell-end, it tends to lower second octave pitch. It is then also true that large sound-holes/mouthpiece windows need a more extreme taper of the bore to stay in tune between the octaves. Another practical consequence of a conical bore would be that fingerholes could be made larger without risking a low pitched second octave. Very convenient, as this would produce a louder whistle. This all adds up to the fact that all the parameters of a whistle work together and are inter-dependent, at least to some degree. Change one thing, and all the other parameters will become affected. The perfect whistle would then be a whistle where all the parameters are at their optimum values, which will never happen in real life. What is possible, on the other hand, is to make a whistle where all the parameters are within reasonable values. Let me give an example of a whistle design that would be less than well optimized: Large wall-thickness, large fingerholes and a mouthpiece window having a large area would produce a whistle with poor octave tuning. Now three different parameters are pulling together in the same direction, namely lowering second octave pitch. If whistle designers reckognizes these practical consequences as something they have experienced themselves, it then shows that the above theories holds water. If they wouldn't, then welcome to the world of lunacy. |
|
Making a cavity underneath the windway has the effect of lowering the pitch of the second octave notes, and particurarly that of the second octave D.
This could be useful when second octave pitch is found to be too high when making whistles having a tapered bore.
The rule of thumb is that the amount of cavity volume creates a correspondingly low second octave pitch.
I have found that tapered bores notoriously show up with a second octave pitch so sharp that it makes them unplayable.
A large cavity seems to cure this tendency.
|
|
Undercutting of the fingerholes |
![]() |
The relationship between the cavity underneath the windway, tapered bores and octave tuning
As mentioned before, the wall-thickness of the shaft influences the second octave pitch, in such a way that a great wall-thickness tends to lower the pitch of the
second octave. It is therefore wise to take this fact into account when making conical shafts that causes the second octave go sharp. Such a shaft may require a
cavity volume which is less compared with shafts having a smaller wall-thickness.
|
| | Shop | | Payment/Shipping | | Contact | | About | | Images | | Links | | Reviews | |