The law of Conservation of Mechanical Energy states that if no external forces act (or the work done by them is zero) and the internal forces are conservative, the mechanical energy of the system remains constant.

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What is conservation of mechanical energy?

The Law of Conservation of Mechanical Energy states that in a closed system where only conservative forces (such as gravity or spring force) are acting, the total mechanical energy of the system remains constant. This means that the sum of kinetic energy (K.E.) and potential energy (P.E.) remains unchanged over time, provided no external or non-conservative forces (like friction or air resistance) do work on the system.

What kind of question can we solve, and what kind of question can we not, using the law of Conservation of Mechanical Energy?

If non-conservative forces do work on the system or external forces do work on the system, we cannot use the conservation principle of total mechanical energy.

Suppose work done by non-conservative forces equals zero. In that case, work done by external forces equals zero, and internal forces operating within the system are conservative; then and only can we use the principle of conservation of total mechanical energy.

The law of Conservation of Mechanical Energy: Evidence through examples

Example 1: Freely falling object near the earth’s surface

Suppose a body of mass m is falling from rest near the earth’s surface. Initially (e = 0), it was at point A, at a height H above the earth’s surface.

Considering (earth + body) as a system and ground surface is considered a reference line. When the body is at point A, the total mechanical energy of the system is

"Diagram of a freely falling object illustrating the law of conservation of mechanical energy. A mass (m) is shown at two positions: Point A at height H with initial velocity v = 0, and Point B at a lower height h with velocity v. The equation below the diagram represents the total mechanical energy at Point A, showing that kinetic energy (KE) is zero while potential energy (PE) is mgH, thus maintaining total mechanical energy as mgH.

But at time t, the body reaches point B, the kinetic energy of the body increases, and the system’s potential energy decreases (because h < H). So, we see that the gain in the body’s kinetic energy is equal to the loss in potential energy of the system.

Mathematical equation representing the total mechanical energy at point B in a freely falling object system. The equation states that the total mechanical energy (TME) at point B is the sum of kinetic energy 1 2 𝑚 𝑣 𝐵 2 2 1 ​ mv B 2 ​ and potential energy 𝑚 𝑔 ℎ mgh, demonstrating the conservation of mechanical energy during free fall 

According to the principle of conservation of energy :

Mathematical derivation of the conservation of mechanical energy for a freely falling object. The equation shows that the total mechanical energy at point B is equal to the total mechanical energy at point A. It further demonstrates that the gain in kinetic energy 1 2 𝑚 𝑣 𝐵 2 2 1 ​ mv B 2 ​ is equal to the loss in potential energy ( 𝑚 𝑔 𝐻 − 𝑚 𝑔 ℎ ) (mgH−mgh), reinforcing the principle of energy conservation

Example 2: A mass attached to a spring oscillating on a smooth surface

Consider a body moving with speed v0 on a smooth horizontal surface. As the body of mass m moves further, spring compresses. We are inserted to calculate the maximum compression produced in the spring.

"Two diagrams illustrating the motion of a block of mass 𝑚 m attached to a spring with spring constant 𝑘 k. In Fig.-1, the block moves with an initial velocity 𝑣 0 v 0 ​ toward the compressed spring, which has a natural length ℓ 0 ℓ 0 ​ . In Fig.-2, the block has compressed the spring to its maximum displacement 𝑥 𝑚 𝑥 x mx ​ , storing potential energy in the spring. The setup demonstrates the conservation of energy as kinetic energy is converted into elastic potential energy.

 Assuming block of mass m and spring as a system.

 At the moment of maximum compression, the body’s speed becomes zero. Hence we see that the K.E. of the body decreases and the P.E. of the system increases.

So, loss in K.E. of the body is equal to gain in elastic potential energy.

According to the principle of conservation of TME.

"Mathematical derivation of the principle of conservation of total mechanical energy (TME) for a mass-spring system. The equation states that the final total mechanical energy ( 𝑇 𝑀 𝐸 𝑠 𝑦 𝑠 TME sys ​ ) is the sum of the kinetic energy ( 𝐾 𝐸 KE) of the body and the potential energy ( 𝑃 𝐸 PE) of the system. The derivation equates the initial kinetic and potential energy to the final energy, demonstrating how the loss in kinetic energy of the moving mass is converted into the gained potential energy stored in the spring.

The law of Conservation of Mechanical Energy: Equation

According to the work-energy theorem, as we know, the work done by all the forces equals the change in the kinetic energy.

Hence we can write,

"Equation representing the work-energy theorem, which states that the work done by conservative forces ( 𝑊 conservative W conservative ​ ), non-conservative forces ( 𝑊 non-conservative W non-conservative ​ ), and external forces ( 𝑊 external W external ​ ) is equal to the change in kinetic energy ( 𝐾 𝑓 − 𝐾 𝑖 K f ​ −K i ​ ). This equation describes how different types of forces contribute to the energy changes of a system.

 

Here, the three terms on the left denote the work done by the conservative internal forces, non-conservative internal forces, and external forces.

As we know, Equation representing the work done by conservative forces ( 𝑊 𝑐 W c ​ ), which is equal to the negative change in potential energy ( − ( 𝑈 𝑓 − 𝑈 𝑖 ) −(U f ​ −U i ​ )). This equation expresses the relationship between work and potential energy in a system.

Here, U stands for the potential energy of the system.

Now from (1) & (2),

Equations representing the relationship between internal work ( 𝑊 𝑖 𝑛 𝑡 W int ​ ), external work ( 𝑊 𝑒 𝑥 𝑡 W ext ​ ), kinetic energy ( 𝐾 K), and potential energy ( 𝑈 U). The second equation expresses the principle of total mechanical energy (T.M.E) in a system, showing that the sum of work done internally and externally results in the change of total mechanical energy.

Where T.M.E. = K + U is the total mechanical energy.

If the internal forces are conservative but external forces act on the system and they do work,   then from equation (3) we can write,

This equation represents the work done by external forces ( 𝑊 𝑒 𝑥 𝑡 W ext ​ ) in a system. It states that the external work is equal to the change in total mechanical energy (T.M.E) of the system.

Therefore, we can write that the work done by external forces equals the change in the total mechanical energy of the system.

Here equation (4) is a mathematical form of energy conservation.

The Law of Conservation of Mechanical Energy: Solved Problems

Example 1: Finding work done by air friction

A body dropped from height h reaches the ground with speed  . Calculate the work done by air friction.

In above question  . Air friction is a non-conservative force. So, we cannot use the principle of conservation of total mechanical energy.

In this condition, we should use, work-energy theorem,

This equation represents the Work-Energy Theorem, which states that the change in kinetic energy 

Example 2: Finding spring constant

A block of mass m moving at a speed v compresses a spring through a distance x before its speed is halved. Find the spring constant of the spring.

The image consists of two diagrams showing a block of mass 𝑚 m moving on a smooth surface while attached to a horizontal spring fixed to a wall

 Let the system is (spring + block)

Here, The equation in the image represents the work done by non-conservative forces in a system

 Internal force (spring force) is conservative.

So, we must use the principle of conservation of total mechanical energy.

The equations in the image describe the principle of total mechanical energy (T.M.E.) in a system 

 Because, When both external work and additional work are zero, the total mechanical energy remains constant.   in above example.

Example 3: Freely falling object, Speed and height calculations

A particle is released from height H. At a certain height from the ground, its kinetic energy is twice its gravitational potential energy. Find the speed of particles and height at that moment.

Ans: Considering particles and earth as a system;

Energy conservation equation with kinetic and potential energy, solving for final velocity in terms of gravitational acceleration and height.

Also, Final kinetic energy is twice the final potential energy.

Derivation showing ℎ = 𝐻 3 h= 3 H ​ using kinetic and potential energy equations.

 Example 4: Finding work done using the conservation of energy approach

Under the action of force, 2 kg body moves such that its position x varies as a function of time given by ; Equation: 𝑥 = 𝑡 3 3 x= 3 t 3 ​ .x is in meters, t is in second. Calculate the work done by the force in the first two seconds.

Ans: Considering 2 kg body and the earth as a system. Here, external force does work on the system, Equation: 𝑊 𝑒 𝑥 𝑡 ≠ 0 W ext ​  =0.

Hence, we cannot use the energy conservation principle for this numerical.

So, here we will use work energy theorem,

Work-energy theorem applied, showing kinetic energy change due to external work      

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FAQs on the Law of Conservation of Mechanical Energy

1. What is the Law of Conservation of Mechanical Energy?

According to the Law of Conservation of Mechanical Energy, the sum of kinetic and potential energy, or total mechanical energy, stays constant in a closed system when only conservative forces are at work.

2. What are conservative and non-conservative forces in mechanical energy conservation?

  • Conservative forces (like gravity and spring force) do not dissipate energy and allow energy to be fully recovered.
  • Non-conservative forces (like friction and air resistance) cause energy dissipation, typically as heat or sound, leading to a decrease in total mechanical energy.

3. Why is friction considered a non-conservative force?

Friction is considered a non-conservative force because it converts mechanical energy into heat, which is lost from the system and cannot be fully recovered.

4. Can we apply the Law of Conservation of Mechanical Energy when friction is present?

No, the law only holds when non-conservative forces like friction and air resistance are absent or do no work on the system. If friction is present, mechanical energy is not conserved, and we must use the work-energy theorem instead.

5. How does the law apply to a freely falling object?

As an object falls under gravity, its potential energy (P.E.) decreases while its kinetic energy (K.E.) increases. However, the total mechanical energy (P.E. + K.E.) remains constant, assuming air resistance is negligible.

6. What is an example of mechanical energy conservation in real life?

A pendulum swinging back and forth is a perfect example. At the highest points, it has maximum potential energy and zero kinetic energy. As it swings down, potential energy converts into kinetic energy, keeping the total mechanical energy constant.

7. What happens to mechanical energy in a system with external forces?

If external forces (such as friction or applied forces) do work on the system, mechanical energy is no longer conserved. Instead, part of the energy is transformed into other forms, like heat or sound.

8. How does the law apply to an oscillating spring system?

Kinetic energy and elastic potential energy continually transform into one another in a mass-spring system when the mass oscillates. As long as the system is not subjected to non-conservative forces (such as friction), the total mechanical energy stays constant.

9. Why is the Law of Conservation of Mechanical Energy important in physics?

This law is an essential tenet of physics that aids in the resolution of issues pertaining to dynamics, motion, and energy transfer. By enabling us to equalize the starting and ultimate energy in a system, it streamlines computations in mechanics.

10. How is the Law of Conservation of Mechanical Energy used in problem-solving?

This law explains how energy flows between motion and position, which helps us calculate things like height and speed. In essence, it states that since total energy remains constant, we can forecast an object’s speed or altitude when it is falling or moving. This is quite helpful for things like springs, roller coasters, swings, and free-falling objects.

Mishra V

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