Hydrostatic Force

Hydrostatic power
Summary
This was a lab to find the hydrostatic coerce that is in effect on a partially submerged surface. This was done both experimentally and by employ an equality to calculate the expected hydrostatic pull up given a change in distance. When I had values of hydrostatic ferocity for all of the different weights both experimentally and through calculation, I put these values in a graph to equivalence my results.
There is then a section which shows what errors might buzz off been incurred and ways that these errors can be reduced or take completely after that there is a short conclusion.

Introduction
The accusatory of this lab is to Measure the hydrostatic draw on a partially submerged vertical surface and compare them to their supposed equivalents.

The hydrostatic force that is in effect on a surface impart let you know how much force is required to keep an item that you are submerging in place.

An example of where this would have a practical application is in a water damn. If the hydrostatic force that will be in effect on a damn is not calculated then you would not know how much force the damn would need to be made to cope with.
A further example is in tidal power, the hydrostatic force of the water is handlingd to create energy through use of turbines.




Theory
An object submerged in a fluid will experience a force called the hydrostatic force (Fh) overdue to the weight of the fluid as shown in the diagram below.
The hydrostatic force (Fh) is the product of the pressure at the centroid (?g?)(where? is the parsimony of the fluid, g is gravity and ? is the centroid) and the surface area of the object (A). This gives the form; Fh=?g?A
For a vertical surface (which is the case in this experiment) the centroid can be shown as ?=h2. Putting these two equations unitedly we get Fh=?gh2A which is the formula that I will be using for the theoretical value of hydrostatic force.

For the experimental value
point in time of action
mg
h3
2h3
Fh
h
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