Upon completing this lesson, you will be able to:
In the previous lesson, we introduced kinetic energy $(KE)$ and potential energy $(PE)$. The sum of these two is called the total mechanical energy $(E)$ of a system.
$$ E = KE + PE $$
The principle of Conservation of Mechanical Energy is a powerful rule that applies under specific conditions. To understand it, we must first define conservative forces.
The Principle of Conservation of Mechanical Energy: If the work done on an object in a system is done only by conservative forces, then the total mechanical energy of the system remains constant.
In other words, energy can be converted between kinetic and potential forms, but the total amount $(E)$ does not change.

$$ E_{\text{initial}} = E_{\text{final}}\\KE_i + PE_i = KE_f + PE_f $$
While the conservation of mechanical energy is a conditional rule, it is a specific case of one of the most fundamental and universal laws of nature: The Law of Conservation of Energy.
This law states: Energy cannot be created or destroyed; it can only be transformed from one form into another.
The total energy of an isolated system is always constant. This principle applies to all forms of energy, not just mechanical.
When a ball falls and hits the ground, its mechanical energy seems to disappear. However, it has been converted into other forms: thermal energy (the ball and ground get slightly warmer) and sound energy. The total energy is still conserved.
What happens when non-conservative forces are present?
When dissipative forces are involved, the total mechanical energy is not conserved; it decreases. However, the universal Law of Conservation of Energy still holds. The "lost" mechanical energy has simply been transformed into thermal energy.
We can modify our conservation equation to account for the work done by non-conservative forces $(W_{nc})$.
$$ E_i + W_{nc} = E_f\\KE_i + PE_i + W_{nc} = KE_f + PE_f $$