It's amazing. You are still asking questions about the concept of frames of reference. I say that it is not possible to reconstruct a frame of reference.
But I can let that go, and still show the idea to be wrong.
You can model the conditions of the frame you are trying to reconstruct. The treadmill is a complete failure in this respect. You don't seem to appreciate how illogical your ideas are, so you concentrate on details, as IF the treadmill were a frame of reference. Its a model, and a bad one.
Please do as I suggested. Walk from the floor onto the treadmill from the usually raised end. Your velocity wrt to the ground increases. However, as you look back, you see that the cart is still where it was, and you are in no doubt that is it stationary wrt the ground. See? It's not moving. It would be almost indistinguishable from one on the floor, right next to it.
Why does it do that? Because it essentially ignores the belt. The belt slips under it, because the friction to it is so low.
Wow! Actually, the cart remains stationary, moves "upbelt" or moves "downbelt" slower than the belt (depending on a variety of conditions) because the propeller, driven by the wheels, driven by the belt, creates thrust against the still air, in the opposite direction of the motion of the belt.
There is no automatic "force balance".
Connect it to the belt as you are when moving, and it will go backwards.
Just as, if the cart is traveling downwind on a road, and you connect it to the road, it will stop.
But that is not important, it just shows up another anomaly. It is not a frame of reference, so that really doesn't matter.
Wrong again. Two frames of reference, both valid.
So what does it say? It says that this cart, responds to being driven into a headwind (like you) by driving itself into a minimum energy state.
Actually, unless considerable effort is made to get the belt at just the right incline, the cart will either drive itself off the end against the motion of the belt, or be pushed off the other end. Of course, in the Humberverse, the cart magically balances the forces and remains stationary.
An orange stays on the belt for another reason.
I've not personally observed this phenomenon, but the most likely mechanism for it is that the weight of the orange causes the belt to sag, creating a low spot, so that the orange is continuously rolling downhill, opposing the motion of the belt. Either that, or the whole belt is moving uphill. However, I think for the orange to stay in one place for more than a few seconds, the weight-induced low spot is the most likely explanation.
My cart too. (There are many ways of doing that. Can't you think of any? No?)
Your imaginary cart? Yes there are many ways you could make it stay in one place. The mechanisms explained for the orange would probably work: Take a simple cart with low-resistance wheels, put enough weight on it to create a sag in the belt. Or put a slight incline in the belt (note that in the propeller cart tests, the incline is in the opposite direction, so this is
not how they work). Heck, just build one. You might learn something (then again, if the cart doesn't work the way you expect it to, you will probably decide the cart is wrong).
In wind, if you wear a pair of skates, and launch a parachute so that it carries you down wind. Eventually, you will reach terminal velocity. Strain gauges to the parachute and in the skates, will show forces to be opposite, but at a maximum.That is the real world case for down wind travel.
Amazing! Very simple, and you still managed to get it wrong. Here is how it works in the real world (not the Humberverse). Note that for this analysis, I am assuming travel directly downwind, such that the parachute is acting as a simple drag device and is not generating lift like a sail on a tack, or a rotating propeller. The force on the parachute will be at a maximum when the stationary skater first deploys the parachute and will accelerate the skater. As the speed of the parachute and skater approach the wind speed, the force on the parachute will
decrease. When the force exerted by the wind on the parachute matches the friction of the skates on the ice (very low friction, so this will be slightly less than wind speed), the skater will stop accelerating, and the force on the parachute will be at a
minimum. The frictional forces on the skates increase with the skater's speed. This is
not however, the primary cause of the skater reaching terminal velocity. The primary cause is the inability of the parachute to generate drag force when it is moving at the same speed as the wind.
On the treadmill, the opposite will happen. When you reach 'terminal velocity', you will be stationary as the cart is now. The gauges will show a minimum force. Opposite to the real world, except for the case where you are NOT traveling. That is the correct view of the cart or 'frame', if you must.
Note that with correct analysis of the "skater going downwind" the "real world" and "treadmill" cases are identical. So that we are not comparing apples to oranges, we will assume the treadmill is long enough to allow the parachute and skater become (nearly) stationary and substitute rollerskates (or maybe lollerskates) for ice skates. Ice doesn't bend too well, so it's kind of hard to make a treadmill out of it. Here is what will happen(from the "ground" frame of reference): The skater moving with the treadmill belt deploys the parachute. The parachute, catching the stationary air, slows down the skater The force will be at its
maximum when the chute is first deployed and will decrease as the skater's speed decreases. As the skater slows down to a speed where the drag from the parachute matches the rolling resistance of his skates, which will be almost stationary, but moving slowly in the direction of motion of the belt the force on the parachute will reach a
minimum, just like in the "real world'. Note that the rolling resistance of the skates will be at its maximum when the skater is at "terminal velocity" (almost stationary relative to the ground). This is
not, however, the primary cause for the skater failing to come to a complete stop (relative to the ground). The primary cause is the inability of the parachute to generate any drag when it is not moving.
QED. The frames of reference are equivalent. Yet another epic fail by Humber.
Imagine a small battery powered wind cart, where a motor drives a propellor. What do you think that will do on the treadmill?
The cart it will move relative to the air in the direction the propeller drives it, with almost no effect (assuming good wheels) from the treadmill. What will it do in the Humberverse?