Yeah sure!
F is the force acting in D distance from the center of the lever.
The common version of the law of lever is:
|F||D|=|F_r||D_r|=1
here |F_r| is the sum of the forces from the rest of the system and
|D_r| is the sum of the distances from the rest of the system.
I have more on...
|F||D|=1 is the simplest form of the law of lever in equilibrium.
If |F|=|x-y| and |D|=x+y then |x^2-y^2|=1 is an real hyperbola.
In this case the interaction is repulsive.
If |F|=x-iy and |D|=x+iy then x^2+y^2=1 is an real ellipse or imaginary hyperbola.
In this case the interaction is...
The universe has only one center.
Assume you consider it consisted of N particles.
Every particle represents a force pressing at some position.
Using the rule of lever in equilibrium you can find the center and the central force for the 1st two particles.
That center is a position in which...
I think that a phenomenon in physics cannot be described with differential equation.
If you have dx=Vdt then you have actually differentiated x=Vt assuming V=const.
I just don't know any other way to come up with dx=Vdt except by derivating x=Vt assuming V=const.
This means that your...
I want you to try this dynamical law:
F' = F cos(k) - aD sin(k)
aD' = F sin(k) + aD cos(k)
It is another form of the law of lever, where F and D are the old force and distance, F' and D' are the new force and distance and a is force / distance ratio...
The new forces and distances in closed system are related with the old like this:
NewF= OldF cos - OldD sin and NewD = OldF sin + OldD cos
This makes gravity.
Gravity law is actually the law of lever.
Torque has nothing to do with it. Archimedes' law of lever governs magnitudes only.
F and D can also be colinear and then torq1 = torq2 is trivial case of Ort = Ort yet magnitudes are still related as the law of lever suggests.
Also distance times force equals energy potential times energy: D...
No problem.
As I said earlier the law of lever has this form:
\frac{F_1}{F_2}=\frac{D_2}{D_1}=\frac{M_1}{M_2}
So F_1 = a * M_1 and F_2 = a * M_2.
Done.
Newton only don't pay attention that this 'a' has to be same for the weight and anti-weight and that it's no acceleration at all. You...
No member. All Newton's laws are only special cases of the law of lever.
Take Newton III for instance:
Newton III says: F_a = -F_r
The law of lever says: F_a * D_a = F_r * D_r
So Newton III is special case of the law of lever when D_a = -D_r.
Weights don't compare only on same...
The Earth has position R_e;
The Earth has force F_e in direction of its displacement;
The moon has position R_m;
The moon has force F_m in direction of its displacement;
We assume that F_e and F_m are parallel and opposite;
The center CF can be found like this:
-Switch the forces;
-Draw...
I do know what lever is and my idea of "lever" happens to be the widest and most general one. I think that all is nothing but highly complex lever in equilibrium. Even the Earth and the moon make a lever although there is no rigid bar there to support them. The center of that invisible lever is...
Magnitudes are in equilibrium on distances reciprocally proportional to their weights - The law of lever according to Archimedes.
Where in this statement do you see any rigid bar?
Yes it says extreme force - extreme energy; extreme energy potential - extreme distance but...
Whatever that part of my page says it's not in the context of this topic, right?
Newton's gravity and Coulomb's law don't respect the law of lever!
Prove that wrong or right if you want to...