But Josh, you are unusual.
The whole ski may not support the skier.OK people, of course the whole ski supports a skier. And a skier needs to feel the whole ski through the whole skiing process, and know what's happening with pressure and grip beneath its whole length at all times.
A skier can at the same time conceptualize the base of support (BoS) as a point under the foot. These are not mutually exclusive.
The whole ski may not support the skier.....
So, we're saying that^ is the same as if the ski were on the ground? How do you equate that?....
If BoS is a point, then how is it that a 115mm wide powder ski supplies more support from sinking in powder than a 70mm carving ski?....
Nothing holds up with this concept of BoS as a point. What am I missing?
Well the point model as presented makes no practical sense. It is at odds with the real world. Models have to match the world, not contradict it.CoM to BoS is a conceptual MODEL. It's intentionally simplified. This does not erase the details of the real world experience. Where are the engineers when we need them?
It seems to me the relationship of COM to BOS is off with respect to the ability to direct pressure along the length of the ski, making it exceedingly difficult to accomplish, not a pirouette, a turn.
Well the point model as presented makes no practical sense. It is at odds with the real world. Models have to match the world, not contradict it.
Just go through and try to use your model to match the conditions I pointed out.
Just the fact that ski on edge vs flat is so different should cause you to question the model. Or the flotation issue, or the length.
I’d be shocked if any engineers supported this model even as a concept.
Seems anti-engineering, but they can answer.
You could try to convince me...
Why would “Base of Support” be a point and not an area? Why not call it “Point of Support”?
Point is fine in this context if the model allows for a torque at that point.Well the point model as presented makes no practical sense. It is at odds with the real world. Models have to match the world, not contradict it.
Just go through and try to use your model to match the conditions I pointed out.
Point is fine in this context if the model allows for a torque at that point.
Careful what you ask for.Where are the engineers when we need them?
You mean like a pivot slip?
The goal is to pivot around the very front of the ski.
Don’t know what these questions have to do with it. They’re red herrings. There’s also a logical fallacy in the construct you’ve made, but it’s beyond me. At the least it’s a false equivalence.So James, are you saying that a skier should not pay attention to and control where the feet are relative to the torso? OR conversely, where the torso is relative to the feet? This spatial relationship is an important factor in controlling how the pressure is distributed under the whole ski.
I don't think you mean that.
I'm a mechanical engineer but only a humble novice skier so I won't/can't make any comment as to the validity of the PSIA terminology/skiing technique discussion.
Strictly on the physics though, technically speaking both a "point" concept and what is called a "distributed load" concept are both valid ways of analyzing forces. Intuitively, you can feel that a ski on the snow has ground reaction/frictional forces acting along its length, the distribution is given by some equation as a function of length when viewing the ski from the side and analyzing the loading along the length of the ski, visually represented by the arrows below the skis in this picture:
Such distributed loads however can analytically be resolved into a single discrete point load at some geometrical point along an object, the ski in this case. Here is a link to the math if you're really interested. This is a "Center of Force" of sorts which can change and move around in space as the loading function/profile along the ski changes, semi-similar to how your CoM location can change depending on the position of your body (That is your actual CoM, I'm assuming that the ski terminology is referring to the same thing as physics class). The location and magnitude of this force can then be used in a free body diagram to do analysis, especially in this case to find moment arms/force couples.
So just as the CoM does not describe the location of all the mass in your body being actually located in a single point in space, neither does a resolved distributed load describe all of its integral force being actually located at a single point. They are however still useful concepts in understanding where/how forces are acting.
Now obviously this is a simplification of reality, and the math of a skier moving dynamically in 3-D space down a hill with variable surface interactions and skiing techniques gets very complicated very quickly. Reality is reality and it's always good to take models with a grain of salt. Buttering is certainly a bit of a boundary case with numerous other complicating factors given that the skis are no longer moving in (comparatively) 2-D arcs across the hill. In the instant of that photo though there is still likely a distributed load on the ski tips, albeit over a small area, which can be resolved into a point load that factors into the overall summation of forces which describes the skier's dynamic balance on their tips.
This force is what allows you to stand on your skis as you turn without them sliding endlessly down/across the hill. Whether this resolved point load or a distributed load along the skis is more synonymous with the PSIA BoS concept you're all speaking of I can't say of course, but hopefully that helps.
....I’m saying one should know where the tail of the ski is. And the tip. Skis can’t be reduced to a point under the foot if you’re referencing a base of support.....
Yeah that’s the problem of reducing the resultant force to a point vector, if that’s the term. It’s the result.Adjusting the spatial relationship between the feet (under the back of the arch) and the torso is a cause. It's what the skier does to manage pressure along the length of the ski. The result is pressure moving along the ski, under the shovel to waist to tail or in the other direction or wherever. Cause and effect are not mutually exclusive. They are locked together.
....Finally, and related to this discussion, "direct pressure along the length of the ski" doesn’t tell anyone what to do and is pretty much useless as a teaching aide. It doesn't say anything about where, or when, or what part of the "length of the ski" should get the pressure and it fails to tie the specific technique to any particular purpose or intent. ....
we "direct" pressure toward the outside ski seems to imply that we need to make some kind of active move towards the outside ski, whereas in fact we move inside the turn (incline) as much as is required for balance on the outside ski against the forces of the turn
it’s odd that this so-called “fundamental” describes controlling "the relationship of the center of mass to the base of support" only as it relates to fore-aft pressure regulation (along the length of the ski). In fact, that relationship is the basis for regulation of fore-aft pressure, lateral pressure and overall magnitude of pressure - in other words, that simple relationship is the basis for all pressure control.
Finally, and related to this discussion, "direct pressure along the length of the ski" doesn’t tell anyone what to do and is pretty much useless as a teaching aide. It doesn't say anything about where, or when, or what part of the "length of the ski" should get the pressure and it fails to tie the specific technique to any particular purpose or intent. Because of that, it makes things like inside ski turns and two-footed powder turns seem like mistakes.