According to the law of conservation of energy, in a closed system isolated from its surroundings, the total energy remains constant. Conservative forces follow this principle. In this article, we will explore the concepts of conservative and non-conservative forces.
A conservative force is a type of force where the work done by or against the force on an object moving between two points depends only on the initial and final positions, not the path taken. This property is directly linked to the law of conservation of energy, as energy within the system remains constant.
Examples of Conservative Forces
The formula for a conservative force is derived from the relationship between the force and the potential energy associated with it. A force is conservative if it can be expressed as the negative gradient of a potential energy function.
Formula
F = -∇U
U
with respect to position.A non-conservative force is a type of force where the work done by or against the force depends on the path taken, not just the initial and final positions. Non-conservative forces dissipate mechanical energy from the system, usually as heat, sound, or deformation, and thus, the total mechanical energy is not conserved.
Examples of Non-Conservative Forces
The work done by a conservative force depends only on the initial and final positions of the object and is independent of the path taken. This property is a defining characteristic of conservative forces and is closely related to the concept of potential energy.
Path Independence:
The work done by a conservative force moving an object between two points depends solely on the start and end points. Example: For gravity, the work done to move an object to a certain height depends only on the height difference, not the path.
Potential Energy Relationship:
Work done by a conservative force is equal to the negative change in potential energy (U
) of the system:
W = -ΔU
For example, in a gravitational field:
W = - (Ufinal - Uinitial) = - m g (hfinal - hinitial)
Work Along a Closed Path:
For a closed loop, the total work done by a conservative force is zero:
∮ F ⋅ dr = 0
Energy Conservation:
In a system where only conservative forces act, the total mechanical energy (kinetic + potential) remains constant:
KEinitial + PEinitial = KEfinal + PEfinal
Consider moving an object of mass m
from height h1
to h2
:
W = -ΔU = - m g (h2 - h1)
The work depends only on h1
and h2
, not the path.
The difference between conservative force and non-conservative force are given below-
Aspect | Conservative Force | Non-conservative Force |
---|---|---|
Definition | A force where the work done depends only on the initial and final positions, not the path taken. | A force where the work done depends on the path taken, not just the initial and final positions. |
Energy Conservation | Mechanical energy is conserved in the presence of only conservative forces. | Mechanical energy is not conserved as it is dissipated (e.g., as heat or sound). |
Work Done in a Closed Path | Work done over a closed path is zero. | Work done over a closed path is not zero. |
Associated Potential Energy | Can be associated with a potential energy function. | Cannot be associated with a potential energy function. |
Examples | Gravitational force, electrostatic force, spring force. | Frictional force, air resistance, viscous force. |
Path Dependence | Path-independent; work depends only on displacement. | Path-dependent; work depends on the entire path. |
A conservative force is one where the work done in moving an object between two points depends only on those points, not the path taken. Example: The gravitational force is conservative. When lifting an object to a certain height, the work done against gravity depends only on the height difference, not the path taken. This work is stored as gravitational potential energy, which can be fully recovered if the object returns to its original position.
To determine if a force is conservative: