Work, Energy and Power — JEE Main practice

26 questions

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Sample questions with solutions

Q1 · 2026

Potential energy ( VV ) versus distance ( xx ) is given by the graph. Rank various regions as per the magnitudes of the force ( FF ) acting on a particle from high to low.

  • A.

    FBC>FCD>FDE>FABF_{BC}>F_{CD}>F_{DE}>F_{AB}

  • B.

    FCD>FAB>FBC>FDEF_{CD}>F_{AB}>F_{BC}>F_{DE}

  • C.

    FBC>FAB>FDE>FCDF_{BC}>F_{AB}>F_{DE}>F_{CD}

  • D.

    FCD>FDE>FAB>FBCF_{CD}>F_{DE}>F_{AB}>F_{BC}

Answer: C
  1. The force acting on a particle equals the negative slope of its potential energy versus position graph.
F=dVdxF = -\frac{dV}{dx}
  1. So the magnitude of the force in each region equals the absolute value of the slope between that region's endpoints.
F=V2V1x2x1|F| = \left|\frac{V_2-V_1}{x_2-x_1}\right|
  1. For region ABAB, from (0,0)(0,0) to (1,1)(1,1):
FAB=1010=1|F_{AB}| = \left|\frac{1-0}{1-0}\right| = 1
  1. For region BCBC, from (1,1)(1,1) to (2,4)(2,4):
FBC=4121=3|F_{BC}| = \left|\frac{4-1}{2-1}\right| = 3
  1. For region CDCD, from (2,4)(2,4) to (4,4)(4,4):
FCD=4442=0|F_{CD}| = \left|\frac{4-4}{4-2}\right| = 0
  1. For region DEDE, from (4,4)(4,4) to (6,3)(6,3):
FDE=3464=0.5|F_{DE}| = \left|\frac{3-4}{6-4}\right| = 0.5
  1. Arrange these magnitudes in descending order.
3>1>0.5>0    FBC>FAB>FDE>FCD3 > 1 > 0.5 > 0 \;\Rightarrow\; F_{BC} > F_{AB} > F_{DE} > F_{CD}

Hence, the ranking from high to low is FBC>FAB>FDE>FCDF_{BC}>F_{AB}>F_{DE}>F_{CD}, so the answer is option C.

Q2 · 2026

A body of mass 2 kg is moving along x-direction such that its displacement as function of time is given by x(t)=αt2+βt+γx(t) = \alpha t^2 + \beta t + \gamma m, where α=1 m/s2\alpha = 1 \ m/s^2, β=1 m/s\beta = 1 \ m/s and γ=1 m\gamma = 1 \ m. The work done on the body during the time interval t=2 st = 2 \ s to t=3 st = 3 \ s, is ________ J.

  • A.

    42

  • B.

    24

  • C.

    12

  • D.

    49

Answer: B
  1. Velocity is the rate of change of displacement with time, found by differentiating x(t)x(t).
v(t)=dxdt=2αt+βv(t) = \frac{dx}{dt} = 2\alpha t + \beta
  1. Substitute α=1 m/s2\alpha=1\text{ m/s}^2 and β=1 m/s\beta=1\text{ m/s}.
v(t)=2t+1v(t) = 2t+1
  1. Find the velocity at the start and end of the interval.
vi=v(2)=2(2)+1=5 m/s,vf=v(3)=2(3)+1=7 m/sv_i = v(2) = 2(2)+1 = 5\text{ m/s}, \qquad v_f = v(3) = 2(3)+1 = 7\text{ m/s}
  1. By the work-energy theorem, the work done equals the change in kinetic energy.
W=12m(vf2vi2)W = \frac{1}{2}m(v_f^2-v_i^2)
  1. Substitute m=2 kgm=2\text{ kg}.
W=12(2)(7252)=4925=24 JW = \frac{1}{2}(2)(7^2-5^2) = 49-25 = 24\text{ J}

Hence, the work done on the body is 24 J, so the answer is option B.

Q3 · 2026

Given below are two statements :

Statement I : An object moves from position r1r_1 to position r2r_2 under a conservative force field F\vec{F}. The work done by the force is W=r1r2FdrW=-\int\limits_{r_1}^{r_2} \vec{F} \cdot \overrightarrow{dr}.

Statement II : Any object moving from one location to another location can follow infinite number of paths. Therefore, the amount of work done by the object changes with the path it follows for a conservative force.

In the light of the above statements, choose the correct answer from the options given below :

  • A.

    Statement I is true but Statement II is false

  • B.

    Statement I is false but Statement II is true

  • C.

    Both Statement I and Statement II are false

  • D.

    Both Statement I and Statement II are true

Answer: C
  1. The general definition of work done by a force F\vec F while moving an object from r1\vec r_1 to r2\vec r_2 is the line integral of the force along the path, without any extra negative sign.
W=r1r2FdrW = \int\limits_{r_1}^{r_2}\vec F\cdot d\vec r
  1. This formula applies to both conservative and non-conservative forces. Statement I instead claims W=r1r2FdrW=-\int_{r_1}^{r_2}\vec F\cdot d\vec r, which is incorrect, so Statement I is false.
  2. For a conservative force specifically, the work done equals the negative change in potential energy, and this value depends only on the initial and final positions.
W=r1r2Fdr=(UfUi)W = \int\limits_{\vec r_1}^{\vec r_2}\vec F\cdot d\vec r = -(U_f-U_i)
  1. Since a conservative force satisfies Fdr=0\oint\vec F\cdot d\vec r=0 (zero net work over any closed loop), the work between two fixed points is path-independent.
  2. Statement II claims the work done changes with the path taken for a conservative force — this directly contradicts path-independence, so Statement II is also false. Hence, both Statement I and Statement II are false, so the answer is option C.

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