Sign in
12thPass logo
New chatPYQ LibraryDoubtsRank report
Sign in to see Recents

Your guest activity stays on this device

Sign in to save progress →
Sign in

Rotational Motion question

2020 · 7 Jan · Shift 2 · Q39
Guest · filters and generic practice availableBrowsing as a guest · PYQ filters and generic practice are available. Sign in only for personalised features and saved progress.
  1. PYQ Library
  2. /JEE Main
  3. /Physics
  4. /Rotational Motion
  5. /2020 · 7 Jan · Shift 2 · Q39

Rotational Motion question

2020 · 7 Jan · Shift 2 · Q39

JEE MainPhysicsRotational MotionNumerical+4 / −1
JEE Main 2020 (Online) 7th January Evening Slot Physics - Rotational Motion Question 155 English Consider a uniform cubical box of side a on a rough floor that is to be moved by applying minimum possible force F at a point b above its centre of mass (see figure). If the coefficient of friction is μ\muμ= 0.4, the maximum possible value of 100 ×ba{b \over a}ab​ for box not to topple before moving is .......
Numerical answer
View written solutionFree

Correct answer: 50

  1. Set up the geometry and forces

    A uniform cube of side aaa rests on a rough horizontal floor.

    • Weight: mgmgmg, acting through the centre of mass.
    • A horizontal force FFF is applied at a point whose height above the centre of mass is bbb.
    • Coefficient of friction with floor: μ=0.4\mu = 0.4μ=0.4.

    Since the centre of mass is at height a/2a/2a/2 above the floor, the force is applied at height h=a2+bh = \frac{a}{2} + bh=2a​+b above the floor.

  2. Condition for the box to start sliding

    The minimum force needed to make the box move by sliding is when static friction reaches its limiting value: Fslide=μmgF_{\text{slide}} = \mu mgFslide​=μmg

  3. Condition for the box to topple

    The box will begin to topple about the lower edge on the side of pulling when the torque of FFF about that edge equals the restoring torque of weight.

    Taking moments about the bottom edge on the tipping side:

    • Moment arm of FFF: h=a2+bh = \dfrac{a}{2}+bh=2a​+b
    • Moment arm of mgmgmg: a2\dfrac{a}{2}2a​

    So, at toppling threshold, Ftopple(a2+b)=mg(a2)F_{\text{topple}}\left(\frac{a}{2}+b\right)=mg\left(\frac{a}{2}\right)Ftopple​(2a​+b)=mg(2a​)

    Hence, Ftopple=mg (a/2)(a/2+b)F_{\text{topple}}=\frac{mg\,(a/2)}{(a/2+b)}Ftopple​=(a/2+b)mg(a/2)​

  4. For the box to move without toppling first

    Sliding must occur before toppling, so the sliding force should be less than or equal to the toppling force: Fslide≤FtoppleF_{\text{slide}} \le F_{\text{topple}}Fslide​≤Ftopple​

    Substituting, μmg≤mg (a/2)(a/2+b)\mu mg \le \frac{mg\,(a/2)}{(a/2+b)}μmg≤(a/2+b)mg(a/2)​

    Cancel mgmgmg: μ≤a/2a/2+b\mu \le \frac{a/2}{a/2+b}μ≤a/2+ba/2​

  5. Substitute μ=0.4\mu = 0.4μ=0.4

    0.4≤a/2a/2+b0.4 \le \frac{a/2}{a/2+b}0.4≤a/2+ba/2​

    Rearranging: 0.4(a2+b)≤a20.4\left(\frac{a}{2}+b\right) \le \frac{a}{2}0.4(2a​+b)≤2a​

    0.2a+0.4b≤0.5a0.2a + 0.4b \le 0.5a0.2a+0.4b≤0.5a

    0.4b≤0.3a0.4b \le 0.3a0.4b≤0.3a

    b≤0.75ab \le 0.75ab≤0.75a

  6. But the point of application must lie on the box

    Since the cube has side aaa, the highest possible point on the box is its top face, which is at height aaa above the floor.

    The centre of mass is at height a/2a/2a/2, so the maximum physically possible value of bbb is bmax⁡=a−a2=a2b_{\max}=a-\frac{a}{2}=\frac{a}{2}bmax​=a−2a​=2a​

    This is less than 0.75a0.75a0.75a, so the no-toppling condition is automatically satisfied for all possible points on the box.

    Therefore, the maximum possible value is bmax⁡=a2b_{\max}=\frac{a}{2}bmax​=2a​

  7. Required quantity

    100×ba=100×12=50100\times \frac{b}{a}=100\times \frac{1}{2}=50100×ab​=100×21​=50

Final Answer

50\boxed{50}50​

PreviousNext

More from Rotational Motion

  • Mass per unit area of a circular disc of radius a depends on the distance r from its centre as σ(r) = A + Br . The moment of inertia of the disc about the axis, perpendicular to the plane and assing through its…2020 · MCQ
  • Consider a uniform rod of mass M = 4m and length ℓ pivoted about its centre. A mass m moving with velocity v making angle θ=4π​ to the rod's long axis collides with one end of the rod and sticks to it. The angular…2020 · MCQ
  • A uniform sphere of mass 500 g rolls without slipping on a plane horizontal surface with its centre moving at a speed of 5.00 cm/s. Its kinetic energy is :2020 · MCQ
  • A body of mass m = 10 kg is attached to one end of a wire of length 0.3 m. The maximum angular speed (in rad s–1) with which it can be rotated about its other end in space station is : (Breaking stress of wire = 4.8 × 107 Nm–2 and area of…2020 · Numerical
  • One end of a straight uniform 1m long bar is pivoted on horizontal table. It is released from rest when it makes an angle 30º from the horizontal (see figure). Its angular speed when it hits the table is given as n​ s-1, where n is… Includes diagram2020 · Numerical
  • Three solid spheres each of mass m and diameter d are stuck together such that the lines connecting the centres form an equilateral triangle of side of length d. The ratio I0/IA of moment of inertia I0 of the system about an axis passing… Includes diagram2020 · MCQ
  • A uniformly thick wheel with moment of inertia I and radius R is free to rotate about its centre of mass (see fig). A massless string is wrapped over its rim and two blocks of masses m1 and m2 (m1 > m2) are attached to the ends of the… Includes diagram2020 · MCQ
  • A thin circular plate of mass M and radius R has its density varying as ρ(r) = ρ 0r with ρ 0 as constant and r is the distance from its centre. The moment of Inertia of the circular plate about an axis perpendicular to the…2019 · MCQ