Determining Effective Force of Gravity

AI Thread Summary
To find the effective force of gravity at a specific latitude, it's essential to consider the components of gravitational force and centripetal acceleration. At 45 degrees latitude, the weight of the object (W = mg) acts towards the center of the Earth, while the normal force (N) acts perpendicular to the surface. The centripetal acceleration can be expressed as a = ω²Rcos²θ, where R is the Earth's radius and θ is the latitude. By analyzing the radial components, the equation N_r = mg - mω²Rcos²θ can be derived, allowing for the calculation of the normal force and effective weight. Understanding these vector relationships is crucial for solving the problem effectively.
ffanxii4ever
Messages
1
Reaction score
0
How do you find the effective force of Gravity when at a particular latitude?

I keep trying to figure it out, but I can't seem to wrap my head around it. I understand that some small portion of the force of gravity goes towards your centripetal acceleration at certain latitudes, but I can't seem get the idea, since you seem to have three unknowns, but only two equations.

For example (45 degree latitude):

You are not moving in the y-direction, so the y-component of your weight must be equal to the y-component of your normal force; http://ffanxii4ever.googlepages.com/hp1.bmp/hp1-medium;init:.jpg
and then the net force in the centripetal acceleration is:
http://ffanxii4ever.googlepages.com/hp2.bmp/hp2-medium;init:.jpg

But you only have these two equations, but you have three variables, the normal force, the acceleration of gravity (and as a result the force of gravity) and the angle that the normal force is at (it is offset from the force of gravity).

Does anyone have any idea as to what I am missing, that is making me incapable of understanding this? Thanks.
 
Last edited by a moderator:
Physics news on Phys.org
There are only two forces acting on the object: The weight, W = mg, which acts toward the center of the Earth, and the normal force, N. You also know the acceleration, a = ω²r = ω²Rcosθ, which acts toward the axis of rotation. (R is the radius of the Earth.)

You have all you need to solve for the normal force (which gives you the effective weight of the object). Think vectorially:
\vec{W} + \vec{N} = m\vec{a}

Looking at just the radial components, you have:
-mg + N_r = -m\omega^2R\cos^2\theta

Or:
N_r = mg -m\omega^2R\cos^2\theta
 
Thread 'Question about pressure of a liquid'
I am looking at pressure in liquids and I am testing my idea. The vertical tube is 100m, the contraption is filled with water. The vertical tube is very thin(maybe 1mm^2 cross section). The area of the base is ~100m^2. Will he top half be launched in the air if suddenly it cracked?- assuming its light enough. I want to test my idea that if I had a thin long ruber tube that I lifted up, then the pressure at "red lines" will be high and that the $force = pressure * area$ would be massive...
I feel it should be solvable we just need to find a perfect pattern, and there will be a general pattern since the forces acting are based on a single function, so..... you can't actually say it is unsolvable right? Cause imaging 3 bodies actually existed somwhere in this universe then nature isn't gonna wait till we predict it! And yea I have checked in many places that tiny changes cause large changes so it becomes chaos........ but still I just can't accept that it is impossible to solve...
Back
Top