It was Dave that suggested that R>mg (statically), so I pointed out that it means that m must then fly away (in direction of R). Dave got it wrong.
It seems you have not read what I have written at all. So I repeat.
You are correct. I did not read the rest of your post.
When I find an error like that in the
first line of a post, I see no point in reading further. At least not until the error is addressed. For much the same reason I am not addressing the rest of your most recent post to me until you understand your assertion is
wrong.
You claim that Dave Rogers is wrong.
As has been pointed out to you (repeatedly), you are treating this as if it were a static scenario, instead of a dynamic one.
I'm going to go into more depth on this.
I apologize in advance, the formulae I'm going to be using are a little more advance than the elementary school level F = ma I used previously.
Now we are moving into the realm of high-school physics.
I understand that this may be a little too complicated for the children you write your papers for to understand. Accordingly, I'm going to explain everything as weel as I possibly can. If said children still have trouble understanding what is going on, please direct them to talk to a local high-school physics teacher.
And now I shall introduce the equations that shows Dave Rogers is correct, and you are wrong:
Newton's Second Law of Motion: F = ma
where
F = force
m = mass
a = acceleration
This formula gives the relationship between the force acting on a mass, and the acceleration that the mass undergoes as a result of the force.
Uniformly accelerated rectilinear motion: v = v0 + at
where: v = instantaneous velocity
v
0 = initial velocity
a = acceleration
t = time
This is the equation for determining the velocity of a mass that is undergoing acceleration. Here we need to note again that acceleration and velocity are
vectors. A vector is something that has both magnitude (numerical value) and direction. For comparison, a scalar has only magnitude (time is a scalar)
This formula looks complicated, but don't be put off by appearances, children!
It is very straightforward to derive.
You know that the velocity of an object can be determined from its acceleration, right?
If a car takes off from a stationary starting point, and accelerates at a constant rate (which we shall call "a"), we can find the cars velocity from the length of time the car is accelerating. v = at.
To verify that this is true, look at the dimensions:
Acceleration has dimensions of (length/time/time), or (length/time
2).
Time has the dimension of (time).
Thus, av has dimensions (length/time
2)*(time). One of the (time) units cancels, leaving you with dimensions (length/time). This is velocity!
(As a side note: position can also be determined, but the formula is not at2, as you might guess based on dimension. Instead, position requires integration. Integration is a little too advanced for our discussion today, so you'll just have to take my word on it that position is determined from x = 0.5*at2. Towards the end of high school you may get into calculus, and be able to derive this for yourselves.)
But what happens if the car is already moving when it begins to accelerate?
Uh oh! How do we account for
that?
Don't worry, it's easy! This is the great thing about
Dynamics. It allows you to perform calculations based on moving objects. Because not everything is stationary, kids.
In fact, accounting for initial motion is ridiculously simple. We just add it into the equation we determined above.
If you recall , we derived the equation v = at for a car accelerating at a constant rate from a stationary start.
If the car is moving before it begins accelerating, it will have some initial velocity. We will call this initial velocity v
0, and add it into out equation.
Thus, we get v = v
0 + at.
See? Easy and straightforward. Nothing complicated!
Now let's apply it to the falling upper section of Heiwa's tower as it impacts the lower section and experiences a resistance force due to the impact.
For simplicity's sake, we will assume the resistance force is constant (in reality, it will not be, since the tower is not of homogeneous
(<-- New word! It means the same everywhere. For example, Jello is homogeneous. It is Jello everywhere. Building are not homogeneous. There are floors, trusses, beams, open spaces, etc which are not distributed in an even mixture. Rather, a cross-section of a tower will show steel in some places, concrete in others, open space in still other locations, but none of it is mixed together uniformly))
Now, we know the upper block it falling.
It's not hard to figure out. It must be falling, because the lower block can't leap up to meet it (being fixed tot he ground and all), and it is coming into contact with the lower section. Plainly, it must be moving.
So we know it has some initial velocity, v
0.
Now the fact that velocity and acceleration are vectors come into play. Let us assume that upwards is the positive direction. Thus, any accelerations, forces or velocities acting upwards are positive, and any acting downwards are negative.
Since the upper block is falling downwards, its initial velocity is negative. So we will write -v
0.
As a side note, it is possible to determine this initial velocity. The formula is v0 = (2ad)0.5.
where d is the distance traveled. Under gravity, the acceleration will be -g (negative because it acts downwards)
This is another equation requiring calculus, and so the derivation is a little too advanced for our audience today. But feel free to ask a high school math or physics teacher to show you. Oh, and the exponent of 0.5 means the same as a square-root sign.
So now we have a falling mass whose velocity can be determined by:
v = at - v
0 = at - (2gd)
0.5
Now we need to find the acceleration imparted on the falling mass.
If you recall, we assumed the lower section of the tower would provide a constant resistance force. We will call this force R. If you recall from before, force = mass*acceleration. Thus, since the force is a resistance, we can write:
R = ma.
Being a resistance, this force will act against the motion of the upper block. Since the upper block is moving downwards, the resistance force will act upwards, and thus be positive.
Since R is positive, it follows that the acceleration it imparts on the falling mass is positive as well. This is obvious from the equation (R = ma), since mass cannot be negative, thus R and m must have the same direction.
We can now re-arrange the force equation (R = ma) to find a.
Doing so gives us: a = R/m.
We can now plug the acceleration back into our velocity formula. We get:
v = Rt/m - (2gd)
0.5.
But wait! We are still missing one component! We determined acceleration based on the resistance force alone. But we overlooked the acceleration due to gravity! We accounted for it in determining the initial velocity, but not in the instantaneous velocity calculation!
This is a major point, and I hope you caught onto it without me telling you! You have to account for
all the forces acting on an object when you are determining its resultant motion. Otherwise all your calculations are meaningless!
And there are
two accelerating forces acting on the falling mass. There is the upward-acting resistance force. but there is still the downward-acting gravity force! We have to account for both. Fortunately, gravity is as easy to account for as R was. In fact, it is the same equation, only instead of being R = ma, it is F = -mg where g is acceleration due to gravity and F is the force exerted by gravity. We can re-arrange this as we did with the resistance force, and write: g = -F/m. Remember that it is negative, since gravity acts downwards.
v = Rt/m -Ft/m - (2gd)
0.5 = (R - F)t/m - (2gd)
0.5
The velocity of the upper block is determined from the initial velocity of the upper block added to the acceleration imparted by the resistance force and the acceleration due to gravity.
Now let's look at the same three cases we look at earlier, this time using the approach of dynamics instead of the more simple Newton's Second Law approach.
For simplicities sake, I'm going to go back and replace (2gd)
0.5 with the simpler to write v
0. Otherwise the equation will look messy and confusing. Since the only reason for including it is to show that there is initial velocity, there's no reason to clutter the equation by including the method of calculation initial velocity.
So we have
v = (R - F)t/m - v0
1) R = -F (forces R and F are equal in magnitude and opposite in direction),
2) R < -F (force R is less in magnitude and opposite in direction to force F),
3) R > -F (force R is greater in magnitude and opposite in direction to force F)
Starting with scenario 1):
R = -F
v = (R - F)t/m - v0
We can replace R with -F, and we get
v = (-F - F)t/m - v0
But -F - F is zero, so the equation comes out to:
v = v0
Therefore if the resistance force is equal to the force due to gravity, the falling block will continue to move downwards at a constant velocity, v0. This velocity can be determined from (2gd)0.5, where d is the distance the upper block fell before it impacted the lower section.
Now on to scenario 2):
R < -F
v = (R - F)t/m - v0
Since R is less than -F, the function R - F will yield a resultant force equal to R - F. This resultant force will be (magnitude of R) less than (magnitude of F), and negative in direction (eg. if R = 3 and F = -5, R - F = -2). We will call this resultant force B.
v = -Bt/m - v0
Therefore if the resistance force is less than the force due to gravity, the falling block will continue to accelerate downwards with an acceleration rate of less than that of gravity. This, by the way, is what was observed on September 11, 2001.
Finally, scenario 3):
R > -F
v = (R - F)t/m - v0
Since R is greater than -F, the function R - F will yield a resultant force equal to R - F. This resultant force will be (magnitude of F) less than (magnitude of R), and positive in direction (eg. if R = 5 and F = -3, R - F = +2). We will call this resultant force C.
v = +Ct/m - v0
Therefore if the resistance force is greater than the force due to gravity, the falling block will accelerate upwards at a constant rate.
But now things get interesting.
If the upper block is not moving when this resistance force is applied, it will indeed move upwards. BUT IT IS ALREADY MOVING DOWNWARDS AT SOME INITIAL VELOCITY v0!.
The acceleration due to the resistance will act opposite to the direction of motion, slowing the falling upper section down.
IT WILL NOT SHOOT INTO THE AIR! At least, not until the downward motion has been slowed to a stop.
And after that, the situation is static, and the lower section would only provide a resistance force equal to the now-static load of the upper section. Enough to counter the weight of the upper section (mg), nothing more. Doing otherwise would contravene physics.
Besides, if the upper block moves away from the lower section, it is no longer in contact and thus the lower section has no way of applying the resisting force to it!
--- --- --- --- ---
In summary, Dave Rogers is
right when he says:
You've demonstrated that A*S > M1g, which was never in doubt. You've made no attempt to determine F1, and you've asserted that it's equal to M1g. If that were the case, the falling block would fall all the way to the ground at constant speed, therefore the collapse wouldn't arrest. Clearly you have no idea what the magnitude of the friction and entanglement force is, so you have no grounds for claiming it would necessarily arrest the collapse.
and you, Heiwa, are
wrong in saying:
Sorry, F1 cannot be bigger than M1g, because then the latter would fly up into the sky.
I have now proven it using Newton's second Law
and[i/] using dynamics of motion!
As I said, I'm not reading the rest of your post when your opening line contains an error so egregious my 10-year-old nephew could spot it.
And shame on you for trying to pass off your incompetent physics on innocent children!
I only hope your target audience is older than 10, so that they at least have the knowledge to see your mistakes.
YOU ARE WRONG!
And if you are wrong on so basic a calculation, why should the rest of us waste time with the rest of your claims?
Fix this error,and then we can move onto the next issue.
No wonder you have no concept of the intricacies of scaling.