Circular Motion — JEE Main practice

15 questions

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Sample questions with solutions

Q1 · 2026

Two cars A and B each of mass 10310^3 kg are moving on parallel tracks separated by a distance of 1010 m, in same direction with speeds 7272 km/h and 3636 km/h. The magnitude of angular momentum of car A with respect to car B is ________ J·s.

  • A.

    3.6×1053.6\times10^5

  • B.

    10510^5

  • C.

    3×1053\times10^5

  • D.

    2×1052\times10^5

Answer: B
  1. Convert both speeds into SI units.

    vA=72×518=20 m/sv_A=72\times\frac{5}{18}=20\ \mathrm{m/s} vB=36×518=10 m/sv_B=36\times\frac{5}{18}=10\ \mathrm{m/s}
  2. Since both cars move in the same direction, the relative velocity of car A with respect to car B is

    vAB=vAvB\vec{v}_{AB}=\vec{v}_A-\vec{v}_B

    Therefore,

    vAB=2010=10 m/sv_{AB}=20-10=10\ \mathrm{m/s}
  3. The angular momentum of a particle about a point is given by

    L=r×p\vec{L}=\vec{r}\times\vec{p}

    where p=mv\vec{p}=m\vec{v}.

  4. Since the cars move on parallel tracks, the perpendicular distance between their lines of motion is

    r=10 mr_\perp=10\ \mathrm{m}

    Hence,

    L=m.vrelative.rL=m.v_{\text{relative}}.r_\perp
  5. Substitute the given values.

    L=(103)×10×10L=(10^3)\times10\times10 L=105 JsL=10^5\ \mathrm{J\cdot s}
  6. Therefore, the magnitude of the angular momentum of car A with respect to car B is

    105 Js.10^5\ \mathrm{J\cdot s}.
  7. Hence, the correct option is B.

Q2 · 2026

A large drum having radius RR is spinning around its axis with angular velocity ω\omega, as shown in figure. The minimum value of ω\omega so that a body of mass MM remains stuck to the inner wall of the drum, taking the coefficient of friction between the drum surface and mass MM as μ\mu, is:

  • A.

    2gμR\sqrt{\dfrac{2g}{\mu R}}

  • B.

    g2μR\sqrt{\dfrac{g}{2\mu R}}

  • C.

    gμR\sqrt{\dfrac{g}{\mu R}}

  • D.

    μgR\sqrt{\dfrac{\mu g}{R}}

Answer: C
  1. When the drum rotates, three forces act on the body:

    • Weight, Mg\mathrm{Mg}, acts vertically downward.
    • Normal reaction, NN, acts horizontally toward the centre of the drum.
    • Friction, ff, acts upward to prevent the body from sliding downward.
  2. The normal reaction provides the required centripetal force.

    N=MRω2N=M R\omega^2
  3. For the body to remain at rest relative to the rotating drum, the upward friction must balance its weight.

    f=Mgf=\mathrm{Mg}
  4. Static friction can adjust only up to its maximum value.

    fmax=μNf_{\max}=\mu N

    Therefore,

    MgμN\mathrm{Mg}\leq\mu N
  5. Substitute the expression for the normal force.

    Mgμ(MRω2)\mathrm{Mg}\leq\mu(MR\omega^2)

    Cancelling MM,

    gμRω2g\leq\mu R\omega^2
  6. Rearranging,

    ω2gμR\omega^2\geq\frac{g}{\mu R}

    Hence, the minimum angular speed is

    ωmin=gμR.\omega_{\min}=\sqrt{\frac{g}{\mu R}}.
  7. Therefore, the correct option is C.

Q3 · 2026

In case of vertical circular motion of a particle by a thread of length 𝒓𝒓 if the tension in the thread is zero at an angle 3030^\circ shown in figure, the velocity at the bottom point (A)(A) of the circular path is (g=(g = gravitational acceleration))

  • A.

    4gr\sqrt{4gr}

  • B.

    52gr\sqrt{\dfrac{5}{2}gr}

  • C.

    72gr\sqrt{\dfrac{7}{2}gr}

  • D.

    5gr\sqrt{5gr}

Answer: C
  1. Let the point where the tension becomes zero be P.

At point P, the forces acting along the radius are:

  • Tension, (T), directed towards the centre.
  • The radial component of weight, (\mathrm{mg}\sin30^\circ).
  1. Apply the centripetal force equation.
T+mgsin30=mvP2r.T+\mathrm{mg}\sin30^\circ = \frac{\mathrm{m}v_P^2}{r}.

Since the tension is zero,

mg(12)=mvP2r,vP2=gr2.\begin{aligned} \mathrm{mg}\left(\frac{1}{2}\right) &= \frac{\mathrm{m}v_P^2}{r}, \\ v_P^2 &= \frac{gr}{2}. \end{aligned}

[ \qquad\cdots(1) ]

  1. Find the height of point P above the bottom point A.

The centre of the circle is at a height (r) above A.

Point P is an additional height of

rsin30=r2.\begin{aligned} r\sin30^\circ &= \frac{r}{2}. \end{aligned}

Hence,

h=r+r2=3r2.\begin{aligned} h &= r+\frac{r}{2} \\ &= \frac{3r}{2}. \end{aligned}
  1. Apply the law of conservation of mechanical energy between the bottom point A and point P.

Taking the potential energy at A as zero,

12mvA2=12mvP2+mgh.\frac{1}{2}\mathrm{m}v_A^2 = \frac{1}{2}\mathrm{m}v_P^2 + \mathrm{m}gh.
  1. Substitute the values of (v_P^2) and (h).
vA22=12(gr2)+g(3r2)=gr4+3gr2.\begin{aligned} \frac{v_A^2}{2} &= \frac{1}{2}\left(\frac{gr}{2}\right) + g\left(\frac{3r}{2}\right) \\ &= \frac{gr}{4} + \frac{3gr}{2}. \end{aligned} vA2=gr2+3gr=7gr2.\begin{aligned} v_A^2 &= \frac{gr}{2} + 3gr \\ &= \frac{7gr}{2}. \end{aligned}
  1. Therefore,
vA=72gr.\begin{aligned} v_A &= \sqrt{\frac{7}{2}gr}. \end{aligned}
  1. Hence, the correct option is C.

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