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Work Power and Energy question

2025 · 28 Jan · Shift 1 · Q51
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Work Power and Energy question

2025 · 28 Jan · Shift 1 · Q51

JEE MainPhysicsWork Power and EnergyMCQ+4 / −1
A bead of mass ' mmm' slides without friction on the wall of a vertical circular hoop of radius 'RRR' as shown in figure. The bead moves under the combined action of gravity and a massless spring (k) attached to the bottom of the hoop. The equilibrium length of the spring is 'RRR'. If the bead is released from top of the hoop with (negligible) zero initial speed, velocity of bead, when the length of spring becomes 'RRR', would be (spring constant is 'kkk', ggg is accleration due to gravity) JEE Main 2025 (Online) 28th January Morning Shift Physics - Work Power & Energy Question 5 English
  1. A
    2Rg+kR2 m\sqrt{2 R g+\frac{\mathrm{kR}^2}{\mathrm{~m}}}2Rg+ mkR2​​
  2. B
    3Rg+kR2 m\sqrt{3 \mathrm{Rg}+\frac{\mathrm{kR}^2}{\mathrm{~m}}}3Rg+ mkR2​​
  3. C
    2Rg+4kR2 m\sqrt{2 \mathrm{Rg}+\frac{4 \mathrm{kR}^2}{\mathrm{~m}}}2Rg+ m4kR2​​
  4. D
    2gR+kR2 m2\sqrt{\mathrm{gR}+\frac{\mathrm{kR}^2}{\mathrm{~m}}}2gR+ mkR2​​
View written solutionFree

Correct answer: B

  1. Geometry of the setup

    Let the circular hoop have center at the origin, radius RRR.

    • Bottom point of hoop: (0,−R)(0,-R)(0,−R)
    • Top point of hoop: (0,+R)(0,+R)(0,+R)

    The spring is attached at the bottom of the hoop, and its natural length is RRR.

  2. Initial state

    The bead is released from the top of the hoop with negligible speed.

    At the top point, the distance from bottom point to top point is the diameter: li=2Rl_i = 2Rli​=2R

    Since the natural length is RRR, initial extension is xi=li−R=2R−R=Rx_i = l_i - R = 2R - R = Rxi​=li​−R=2R−R=R

    So initial spring potential energy is Us,i=12kR2U_{s,i} = \frac12 kR^2Us,i​=21​kR2

    Initial gravitational potential energy (taking bottom point as reference y=0y=0y=0 if convenient) corresponds to height difference 2R2R2R above bottom, so Ug,i=2mgRU_{g,i} = 2mgRUg,i​=2mgR

    Initial kinetic energy: Ki=0K_i = 0Ki​=0

  3. Position when spring length becomes RRR

    The bead lies on the hoop and is also at distance RRR from the bottom attachment point.

    So the bead is at the intersection of two circles:

    • circle centered at hoop center, radius RRR
    • circle centered at bottom point, radius RRR

    Let the hoop center be (0,0)(0,0)(0,0) and bottom point be (0,−R)(0,-R)(0,−R).

    Then bead coordinates satisfy x2+y2=R2x^2+y^2=R^2x2+y2=R2 and x2+(y+R)2=R2x^2+(y+R)^2=R^2x2+(y+R)2=R2

    Subtracting, y2−(y+R)2=0y^2-(y+R)^2=0y2−(y+R)2=0 y2−(y2+2Ry+R2)=0y^2-(y^2+2Ry+R^2)=0y2−(y2+2Ry+R2)=0 −2Ry−R2=0-2Ry-R^2=0−2Ry−R2=0 y=−R2y=-\frac{R}{2}y=−2R​

    So the bead is at height −R/2-R/2−R/2 relative to the center. Since the top point was at +R+R+R, the vertical drop from top is Δh=R−(−R2)=3R2\Delta h = R-\left(-\frac{R}{2}\right)=\frac{3R}{2}Δh=R−(−2R​)=23R​

    Hence loss in gravitational potential energy is ΔUg=mg⋅3R2\Delta U_g = mg\cdot \frac{3R}{2}ΔUg​=mg⋅23R​

    At this position, spring length equals its natural length RRR, so spring potential energy is zero: Us,f=0U_{s,f}=0Us,f​=0

  4. Apply conservation of mechanical energy

    Since there is no friction, Ki+Ug,i+Us,i=Kf+Ug,f+Us,fK_i+U_{g,i}+U_{s,i}=K_f+U_{g,f}+U_{s,f}Ki​+Ug,i​+Us,i​=Kf​+Ug,f​+Us,f​

    Equivalently, the final kinetic energy equals the decrease in total potential energy: 12mv2=mg(3R2)+12kR2\frac12 mv^2 = mg\left(\frac{3R}{2}\right)+\frac12 kR^221​mv2=mg(23R​)+21​kR2

    Multiply by 2: mv2=3mgR+kR2mv^2 = 3mgR + kR^2mv2=3mgR+kR2

    Therefore, v2=3gR+kR2mv^2 = 3gR + \frac{kR^2}{m}v2=3gR+mkR2​

    So, v=3Rg+kR2m\boxed{v=\sqrt{3Rg+\frac{kR^2}{m}}}v=3Rg+mkR2​​​

  5. Option matching

    This matches Option B.

  6. Comparison with stored answer

    Stored correct answer is B, which agrees with the derived result.

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