wintermute":z473wvzt said:
Time to geek this up a notch. You can have head loss (think of it as loss of pressure - causing you to pull harder for an equivalent air flow) due to bends, kinks, rough surfaces in the air hole, diameter of air hole, the way the air hole opens up at the bit (fast or slow transition), etc. Speed through the chamber and air hole will effect the amount of turbulence and mixing of smoke and air.
So Mr. Pease is abolutely correct - you don't want a wide open bore with theoretically zero head loss. There's a sweet spot somewhere in all the speed, flowrate, pressure turbulence, friction factors that's going to give you an optimal mixture so that you get the right amount of smoke (turbulence and mixing - also providing the necessary amount of air for proper combustion), pressure (sudden drops will cause condensation), etc.
Well said. All the little things, like the shape of the inlet funnel at the tenon end, and the exit funnel at the bit end, and the sudden cooling from expansion outlet, with its commensurate increase in the mixture's density will have an upstream effect on flow. Back pressure is not a very precise term, but serves since it's generally understood. Pipes are deceptively complex systems, and there's often too much reductionism (nothing wrong with reductionism as a first step, but actual understanding of complex systems is wildly incomplete when we stop there) applied in discussions about how they work, what makes one better than another. It's one of the reasons I eschew the term "engineering" when applied to pipe construction. Engineering is a discipline of applied science, not just building something to arbitrary specifications.
When the overall system is considered, the bowl chamber shape and size, the airway's characteristics, the smoker's cadence, the volume of smoke mixture drawn per puff, ambient air temperature and pressure, relative humidity, the packing density of the tobacco, the shape and surface area of the ember cone, the temperature gradient through the system, the change in viscosity of the fluid with respect to many of these variables, and on and on, it's beautifully complex, rapidly becomes a non-linear system of differential equations of several orders—just a bit more complex than a typical hydraulic system. Bernoulli would have had a blast with this stuff.
Fortunately, we don't have to think about this stuff to enjoy a good smoke, and, for most, thinking about it too much would likely become antithetical to that enjoyment, but it's fascinating how something so apparently simple—burning dried leaves in a wooden vessel and sucking the smoke through a straw—can in reality be sufficiently complex to foil attempts at pencil and back of the envelope analysis.