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Work and the Work–Energy Theorem

topicmedium60 MCQ

Work by constant and variable forces and its link to kinetic energy. (Physics › Work, Energy and Power, NEET UG syllabus.)

Practice 10 questionsBack to syllabus~15 min · 60 questions in the bank

What is Work and the Work–Energy Theorem?

Work is done when a force causes a displacement of an object. It is a scalar quantity representing the energy transferred to or from an object by a force.

Key formula / rule: Work done by a constant force

Key points

  • Define work in physics and differentiate it from everyday usage.
  • Calculate work done by a constant force using the dot product.
  • Calculate work done by a variable force using integration.
  • State and apply the Work-Energy Theorem to solve problems involving motion and energy.

Common exam trap

Confusing work with effort or activity; in physics, work requires displacement.

Definitions

Term

Work (Physics)

Meaning

Work is done when a force causes a displacement of an object. It is a scalar quantity representing the energy transferred to or from an object by a force.

Term

Kinetic Energy

Meaning

The energy possessed by an object due to its motion. It depends on the object's mass and speed.

Term

Work-Energy Theorem

Meaning

A principle stating that the net work done by all forces acting on an object is equal to the change in its kinetic energy.

Learning objectives

  • Define work in physics and differentiate it from everyday usage.

  • Calculate work done by a constant force using the dot product.

  • Calculate work done by a variable force using integration.

  • State and apply the Work-Energy Theorem to solve problems involving motion and energy.

  • Identify situations where work done is positive, negative, or zero.

  • Relate work done to changes in kinetic energy.

Formulae

Name

Work done by a constant force

Note

θ is the angle between the force vector F⃗ and the displacement vector d⃗.

Expression

W = F⃗ ⋅ d⃗ = Fd cosθ

Name

Work done by a variable force

Note

Integral is taken from initial to final position. F⃗ is the force vector, d⃗r is the infinitesimal displacement vector.

Expression

W = ∫ F⃗ ⋅ d⃗r

Name

Kinetic Energy

Note

m is mass, v is speed. KE is always positive.

Expression

KE = ½ mv²

Name

Work-Energy Theorem

Note

Wnet is the total work done by all forces acting on the object. KEf and KEi are final and initial kinetic energies.

Expression

Wnet = ΔKE = KEf - KEi = ½ mvf² - ½ mvi²

Prerequisites

  • Basic vector algebra (dot product)

  • Basic calculus (integration)

  • Newton's Laws of Motion

  • Understanding of force and displacement

  • Concept of kinetic energy

Common mistakes

  • Confusing work with effort or activity; in physics, work requires displacement.

  • Incorrectly using the angle θ in W = Fd cosθ (it's the angle between F and d, not necessarily the angle with the horizontal).

  • Forgetting to consider all forces when calculating net work for the Work-Energy Theorem.

  • Applying W = Fd cosθ for variable forces; integration is required for variable forces.

  • Misinterpreting the sign of work (e.g., friction always does negative work if there's relative motion).

  • Not squaring the velocity correctly in the kinetic energy formula (½ mv²).

Keywords

  • Work

  • Force

  • Displacement

  • Constant Force

  • Variable Force

  • Kinetic Energy

  • Work-Energy Theorem

  • Joule

  • Scalar

  • Dot Product

  • Integration

Practice preview

  • When is the work done by a force on an object considered zero?

    easy

  • Which of the following is the SI unit of work?

    easy

  • A force F (in N) acting on a particle varies with its position x (in m) as shown in the graph below. Calculate the work done by the force as the particle moves from x = 0 m to x = 4 m. (The graph shows: From x = 0 to x

    medium