Revision: Work, Power and Energy Physics (Theory) ISC (Science) ISC Class 11 CISCE

The motion of a body in a straight line path is called translational motion.

The energy possessed by a body due to its state of motion is called its kinetic energy.

The kinetic energy of the body due to its vibrational motion is called vibrational kinetic energy or simply vibrational energy.

If a body moves to and fro about its mean position, the motion is called vibrational motion.

The kinetic energy of the body due to rotational motion is called rotational kinetic energy or simply rotational energy.

If a body rotates about an axis, the motion is called rotational motion.

The kinetic energy of the body due to motion in a straight line is called translational kinetic energy.

The rate of doing work is called power.

Power is defined as the rate of doing work or work done per second.

i.e., Power = `("Work done in joule")/("Times in second")`

or,  p = `("W (in joule)")/("t (in second)")`

The energy possessed by a body by virtue of its specific position (or changed configuration) is called the potential energy.

The energy possessed by a body due to its state of rest or of motion, is called mechanical energy.

The energy possessed by a body at rest due to its position or size and shape is called potential energy.

A force that does not follow the conservative force rule, where the work done by or against it depends on the actual path taken.

OR

If work done by or against a force is dependent of the actual path, the force is said to be a non- conservative force.

A force is said to be a conservative force if the work done by or against it is independent of the actual path chosen and depends only on the initial and final positions of the object.

OR

If work done by or against a force is independent of the actual path, the force is said to be a conservative force.

For two colliding bodies, the negative of the ratio of the relative velocity of separation to the relative velocity of approach is called the coefficient of restitution.

A collision in which linear momentum is conserved but kinetic energy is not conserved is called an inelastic collision.

A collision in which both linear momentum and kinetic energy are conserved is called an elastic collision.

A collision as a process where "several objects come together, interact (exert forces on each other) and scatter in different directions."

OR

An event where two or more bodies exert forces on each other in a relatively short time is called a collision.

W = \[\int_{\mathrm{b}}^{\mathrm{a}}\vec{\mathrm{F}}.\overline{\mathrm{ds}}=\int_{\mathrm{b}}^{\mathrm{a}}\mathrm{F}\mathrm{ds}\cos\theta\]

K = \[\frac {1}{2}\] mv²

Kinetic Energy = \[\frac {1}{2}\] mass × (velocity)²

Power P = \[\frac{\text{Work done }W}{\text{Time taken }t}\]

or

P = \[\frac {W}{t}\]

Gravitational Potential Energy U_h = mgh

Statement:

According to the work-energy theorem, the increase in kinetic energy of a moving body is equal to the work done by a force acting in the direction of the moving body.

Proof:

Let a body of mass m be moving with an initial velocity u. When a constant force F is applied to the body along its direction of motion, it produces an acceleration a, and the body's velocity increases from u to v over a distance S.

Force,

F = ma

Work done by the force,

W = F × S

From the equation of motion,

\[v^2=u^2+2aS\Rightarrow S=\frac{v^2-u^2}{2a}\]

Substituting equations (i) and (iii) into (ii):

W = \[ma\times\frac{v^2-u^2}{2a}=\frac{1}{2}m(v^2-u^2)\]

Now,
Initial kinetic energy, K_i = \[\frac {1}{2}\]mu²
Final kinetic energy, K_f = \[\frac {1}{2}\]mv²

Therefore,

W = K_f − K_i

Conclusion:

Work done on the body = Increase in its kinetic energy.
Hence, the work-energy theorem is proved.

• Work done by a constant force is given by W = \[\vec F\] . \[\vec s\] = F s cos⁡ θ; for infinitesimal displacement, dW = \[\vec F\] . d\[\vec x\].
• For a variable force, the standard formula is not applicable; work done is calculated using W = \[\int_{s_{1}}^{s_{2}}\vec{F}\cdot d\vec{s}.\]
• The area under the force-displacement graph represents the work done; for linearly variable force, W = Area APQB.
• Conservative force (e.g., gravity) — work done is path independent; non-conservative force (e.g., friction) — work done is path dependent.
• Mechanical energy is conserved under conservative forces only; W_conservative = −ΔU and W_{non-conservative} = ΔKE + ΔPE.

• S.I. unit: If 1 joule of work is done in 1 second, the power spent is said to be 1 watt.
• C.G.S. unit: The C.G.S. unit of power is erg per second (erg s^-1).
• Relationship between S.I. and C.G.S. units:
   1 W = 1 J s^-1 = 10⁷ erg s^-1
• 1 horse power (H.P.) = 746 W = 0.746 kW

• There are two main types of potential energy: gravitational and elastic.
• Gravitational potential energy is due to height and is given by U = mgh.
• It is zero at infinity and becomes less negative as the distance from Earth increases.
• Elastic potential energy is stored when an object is stretched or compressed.
• Lifting a body stores energy as gravitational potential energy by doing work against gravity.