Work and Energy Physics Notes

Definition and Conditions of Work

  • Definition: Work is done when a force acts on an object and moves it through a distance. It is defined as the product of the magnitude of force and the distance covered in the direction of force:     W=F×SW = F \times S

  • Zero Work Conditions:

    • If displacement S=0S = 0 (e.g., pushing fixed wall).

    • If force F=0F = 0 while moving with uniform velocity.

  • Scalar Nature: Work does not convey directional information and is a scalar quantity.

Work at an Angle and Graphical Calculation

  • Force at an Angle: When force FF acts at an angle θ\theta with the direction of motion, work is done by the component acting along the direction of motion:     W=FScos⁡(θ)W = F S \cos(\theta)

    • Parallel (θ=0∘\theta = 0^\circ): cos⁡(0∘)=1  ⟹  W=FS\cos(0^\circ) = 1 \implies W = F S

    • Perpendicular (θ=90∘\theta = 90^\circ): cos⁡(90∘)=0  ⟹  W=0\cos(90^\circ) = 0 \implies W = 0 (e.g., carrying a load horizontally where the upward force is perpendicular to displacement).

  • Graphical Representation: The area under a force-distance curve represents the work done by that force.


Shaded area under force-distance graph representing work done

Units and Sample Calculations of Work

  • SI Unit: The SI unit of work is the joule (J\text{J}). One joule of work is done when a force of 1 N1\,\text{N} moves a body through a distance of 1 m1\,\text{m} in its direction:     1 J=1 N×1 m=1 N m1\,\text{J} = 1\,\text{N} \times 1\,\text{m} = 1\,\text{N\,m}

  • Larger Units: 1 kJ=103 J1\,\text{kJ} = 10^3\,\text{J}, 1 MJ=106 J1\,\text{MJ} = 10^6\,\text{J}.

  • Worked Examples:

    • 200 J200\,\text{J} of work pushing a carton 5 m5\,\text{m} requires a force of F=200 J5 m=40 NF = \frac{200\,\text{J}}{5\,\text{m}} = 40\,\text{N}.

    • A 65 N65\,\text{N} force pulling a suitcase for 20 m20\,\text{m} at θ=30∘\theta = 30^\circ does work W=65 N×20 m×cos⁡(30∘)=1125.8 JW = 65\,\text{N} \times 20\,\text{m} \times \cos(30^\circ) = 1125.8\,\text{J}.

Concept and Forms of Energy

  • Definition: Energy is the ability of a body to do work. It is a scalar quantity measured in joules (J\text{J}).

  • Energy Transfer: Performing 1 J1\,\text{J} of work spends 1 J1\,\text{J} of energy transferred from one system to another.

  • Basic Mechanical Energy: Mechanical energy consists of:

    • Kinetic energy

    • Potential energy

  • Notable Quantities:

    • Work done by a single beat of the human heart: 0.5 J0.5\,\text{J}

    • Energy of the nuclear bomb dropped on Hiroshima, Japan, in the second world war: 8.0×1013 J8.0 \times 10^{13}\,\text{J}

    • Annual energy output of a power station: 1016 J10^{16}\,\text{J}

Kinetic Energy

  • Definition: Energy possessed by a body by virtue of its motion:     Ek=12mv2E_k = \frac{1}{2} m v^2

  • Derivation Summary: Calculated from work done to bring a body of mass mm moving at velocity vv to rest via opposing force FF across distance SS, using average velocity S=vt2S = \frac{v t}{2} and acceleration slope a=vta = \frac{v}{t}.

  • Example Calculation: A truck of mass m=3000 kgm = 3000\,\text{kg} moving at v=54 km h−1=15 m s−1v = 54\,\text{km\,h}^{-1} = 15\,\text{m\,s}^{-1} has kinetic energy:     Ek=12×3000 kg×(15 m s−1)2=337500 J=337.5 kJE_k = \frac{1}{2} \times 3000\,\text{kg} \times (15\,\text{m\,s}^{-1})^2 = 337500\,\text{J} = 337.5\,\text{kJ}


Velocity-time graph

Potential Energy

  • Definition: Energy possessed by a body by virtue of its position or deformation.

  • Gravitational Potential Energy: Energy stored in an object due to its position relative to the Earth.