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Potential Energy

Table of Contents

  1. Overview
  2. Derivation

Overview

Derivation

We have already seen in the example of the inclined plane that the work is independent of the path and only depends on the height. This fact will now be proven for arbitrary curves in the gravitational field of the earth near its surface.
All quantities to derive a formula for the potential energy.All quantities to derive a formula for the potential energy.
According to the definition of the work, the dot-product can then be written as follows: $$W = \int_{s_1}^{s_2} \vec{F}\cdot\mathrm{d}\vec{s} = \int_{s_1}^{s_2} F\cos\theta\,\mathrm{d}s$$ The correlation between the infinitesimal height $\mathrm{d}h$ and the infinitesimal path $\mathrm{d}s$ is given as: $$\mathrm{d}s = \frac{\mathrm{d}h}{\cos\theta}$$ Inserting this equation and integrating it over the full height leads to $$W = mgh$$ For the potential energy it follows then automatically: $$\boxed{E_\mathrm{pot} = mgh}$$ The important fact is that the amount of energy is independent of the actual path on which the object is lifted. It only depends on the height difference.

Potential Energy


An object lifted upwards in the gravitational field of the earth gains potential energy. The potential energy is independent of the path and simply given as the product of the weight and height: $$E_\mathrm{pot} = mgh$$

Example

A chocolate bar has a weight of 100g and therefore a weight of around 1 N. If we lift it up by 5 m from a table, it gains potential energy of $$E_\mathrm{pot} = mgh = 5\,\mathrm{J}$$

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