If friction between the glass and the table is negligible, the forces would be symmetrical.
But if the friction is high enough to have an effect, it changes things. Friction resists you when you’re speeding the glass up, but helps you when you’re slowing the glass down. As a result the required forces are asymmetrical.
Actually, the problem, here, is that the OP is asking a question based on a totally faulty view of the physics involved. The OP is making some very basic, but false, assumptions, in the question itself. Unless it’s determined what those false assumptions are, there’s no way to properly answer this question. Trying to guess what the OP meant isn’t going to work.
OP, why don’t you try to rephrase it, so we can get an idea of what you believe is happening. Then we can address what’s wrong with your view of the situation you are trying to describe. Then we can maybe answer your actual question.
Oh, I get that, that wasn’t my point. I have two sticking points. One is
This implies that if you keep the scale reading the same, you’ll keep accelerating, which is counterintuitive. I will be the first to admit that intuition is often wrong, but would like to confirm this point so I understand it better. Similarly for
I know that f=ma so that constant force applied to a mass will result in constant acceleration. This is easy to understand in a rocket-in-space situation. But doesn’t dynamic frictional force increase somehow in proportion to the velocity the object is moving?
And further
I interpret that to imply that once I reach my target speed, the scale will show the same force whether I am pushing the box at 1 km/sec or 5 km/sec. That’s the part that is counterintuitive. I think I’ll go get my luggage scale and try this…
Missed the edit window, and I didn’t refresh the page since I left to move snow. It seems the discussion with the OP is already going in the right direction. Ignore my previous post.
The formula for dry kinetic friction is F = mu[sub]k[/sub]*N, where F is the magnitude of the frictional force, mu[sub]k[/sub] is the coefficient of kinetic friction (a constant that depends on the surfaces involved; typical values are in the vicinity of 1 or less), and N is the magnitude of the normal force, the “pushing force” that the two surfaces are exerting on each other (which will typically be equal to the weight of the object, if it’s sitting on a level, non-accelerating surface with no other vertical forces). At least, that’s the simple version: The value of mu[sub]k[/sub] will in reality vary somewhat depending on speed and the normal force and other factors, but it’s pretty close to constant, and it won’t in general vary in the way you expect, anyway.
This is perfect, thank you (#1 is exactly what I described). What is the name for the ‘acceleration time period’ and the ‘deceleration time period’ in this example?