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Rotational Motion question

2019 · 10 Apr · Shift 1 · Q55
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  5. /2019 · 10 Apr · Shift 1 · Q55

Rotational Motion question

2019 · 10 Apr · Shift 1 · Q55

JEE MainPhysicsRotational MotionMCQ+4 / −1
Two coaxial discs, having moments of inertia I1 and I1/2, are rotating with respective angular velocities ω\omegaω 1 and ω\omegaω 1/2 , about their common axis. They are brought in contact with each other and thereafter they rotate with a common angular velocity. If Ef and Ei are the final and initial total energies, then (Ef - Ei) is:
  1. A
    I1ω1224{{{I_1}\omega _1^2} \over {24}}24I1​ω12​​
  2. B
    I1ω1212{{{I_1}\omega _1^2} \over {12}}12I1​ω12​​
  3. C
    38I1ω12{3 \over 8}{I_1}\omega _1^283​I1​ω12​
  4. D
    I1ω126{{{I_1}\omega _1^2} \over {6}}6I1​ω12​​
View written solutionFree

Correct answer: $E_F-E_I=-\DFRAC{I_1\OMEGA_1^2}{24}$, STORED ANSWER A MATCHES ONLY THE MAGNITUDE OF ENERGY LOST, NOT THE ALGEBRAIC VALUE OF $(E_F-E_I)$.

  1. Given data

    Two coaxial discs have:

    • Moment of inertia of first disc: I1I_1I1​
    • Moment of inertia of second disc: I2=I12I_2=\dfrac{I_1}{2}I2​=2I1​​

    Initial angular velocities:

    • First disc: ω1\omega_1ω1​
    • Second disc: ω2=ω12\omega_2=\dfrac{\omega_1}{2}ω2​=2ω1​​

    After contact, they rotate together with common angular velocity ωf\omega_fωf​.

  2. Use conservation of angular momentum

    Since no external torque acts on the system, I1ω1+I2ω2=(I1+I2)ωfI_1\omega_1 + I_2\omega_2 = (I_1+I_2)\omega_fI1​ω1​+I2​ω2​=(I1​+I2​)ωf​

    Substitute the values: I1ω1+I12⋅ω12=(I1+I12)ωfI_1\omega_1 + \frac{I_1}{2}\cdot \frac{\omega_1}{2} = \left(I_1+\frac{I_1}{2}\right)\omega_fI1​ω1​+2I1​​⋅2ω1​​=(I1​+2I1​​)ωf​

    I1ω1+I1ω14=3I12ωfI_1\omega_1 + \frac{I_1\omega_1}{4} = \frac{3I_1}{2}\omega_fI1​ω1​+4I1​ω1​​=23I1​​ωf​

    5I1ω14=3I12ωf\frac{5I_1\omega_1}{4} = \frac{3I_1}{2}\omega_f45I1​ω1​​=23I1​​ωf​

    Cancelling I1I_1I1​: 5ω14=32ωf\frac{5\omega_1}{4} = \frac{3}{2}\omega_f45ω1​​=23​ωf​

    ωf=5ω16\omega_f = \frac{5\omega_1}{6}ωf​=65ω1​​

  3. Initial rotational kinetic energy

    Ei=12I1ω12+12I2ω22E_i = \frac{1}{2}I_1\omega_1^2 + \frac{1}{2}I_2\omega_2^2Ei​=21​I1​ω12​+21​I2​ω22​

    Ei=12I1ω12+12⋅I12⋅(ω12)2E_i = \frac{1}{2}I_1\omega_1^2 + \frac{1}{2}\cdot \frac{I_1}{2}\cdot \left(\frac{\omega_1}{2}\right)^2Ei​=21​I1​ω12​+21​⋅2I1​​⋅(2ω1​​)2

    Ei=12I1ω12+12⋅I12⋅ω124E_i = \frac{1}{2}I_1\omega_1^2 + \frac{1}{2}\cdot \frac{I_1}{2}\cdot \frac{\omega_1^2}{4}Ei​=21​I1​ω12​+21​⋅2I1​​⋅4ω12​​

    Ei=12I1ω12+I1ω1216E_i = \frac{1}{2}I_1\omega_1^2 + \frac{I_1\omega_1^2}{16}Ei​=21​I1​ω12​+16I1​ω12​​

    Ei=8+116I1ω12=916I1ω12E_i = \frac{8+1}{16}I_1\omega_1^2 = \frac{9}{16}I_1\omega_1^2Ei​=168+1​I1​ω12​=169​I1​ω12​

  4. Final rotational kinetic energy

    Ef=12(I1+I2)ωf2E_f = \frac{1}{2}(I_1+I_2)\omega_f^2Ef​=21​(I1​+I2​)ωf2​

    Ef=12(I1+I12)(5ω16)2E_f = \frac{1}{2}\left(I_1+\frac{I_1}{2}\right)\left(\frac{5\omega_1}{6}\right)^2Ef​=21​(I1​+2I1​​)(65ω1​​)2

    Ef=12⋅3I12⋅25ω1236E_f = \frac{1}{2}\cdot \frac{3I_1}{2} \cdot \frac{25\omega_1^2}{36}Ef​=21​⋅23I1​​⋅3625ω12​​

    Ef=3I14⋅25ω1236E_f = \frac{3I_1}{4}\cdot \frac{25\omega_1^2}{36}Ef​=43I1​​⋅3625ω12​​

    Ef=75144I1ω12=2548I1ω12E_f = \frac{75}{144}I_1\omega_1^2 = \frac{25}{48}I_1\omega_1^2Ef​=14475​I1​ω12​=4825​I1​ω12​

  5. Find Ef−EiE_f-E_iEf​−Ei​

    Ef−Ei=2548I1ω12−916I1ω12E_f-E_i = \frac{25}{48}I_1\omega_1^2 - \frac{9}{16}I_1\omega_1^2Ef​−Ei​=4825​I1​ω12​−169​I1​ω12​

    =(2548−2748)I1ω12= \left(\frac{25}{48}-\frac{27}{48}\right)I_1\omega_1^2=(4825​−4827​)I1​ω12​

    =−248I1ω12= -\frac{2}{48}I_1\omega_1^2=−482​I1​ω12​

    Ef−Ei=−I1ω1224E_f-E_i = -\frac{I_1\omega_1^2}{24}Ef​−Ei​=−24I1​ω12​​

  6. Interpretation

    The final energy is less than the initial energy, so energy is lost due to friction during contact.

    Hence, Ef−Ei=−I1ω1224E_f-E_i=-\frac{I_1\omega_1^2}{24}Ef​−Ei​=−24I1​ω12​​

  7. Option check

    The options list only positive values. The correct algebraic value is negative. If the question intended the loss of energy, then its magnitude is: ∣Ef−Ei∣=I1ω1224\left|E_f-E_i\right|=\frac{I_1\omega_1^2}{24}∣Ef​−Ei​∣=24I1​ω12​​ which corresponds to Option A.

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