Q 1 :

A ball of mass (m) 0.5 kg is attached to the end of a string having length (L) 0.5 m. The ball is rotated on a horizontal circular path about a vertical axis. The maximum tension that the string can bear is 324 N. The maximum possible value of angular velocity of the ball (in radian/s) is                     [2011]

[IMAGE 61]

  • 9

     

  • 18

     

  • 27

     

  • 36

     

(4)

Tsinθ=mRω2                          ...(i)

Tcosθ=mg                               ...(ii)

Dividing (ii) by (i), we get

tanθ=ω2Rg    ω=Rgtanθ

[IMAGE 62]

Clearly, ω is maximum when tanθ is maximum, i.e., θ=90°

[IMAGE 63]

So, Tsin90°=mRω2

T=mLω2  [Here, R=L]

ω=TmL=3240.5×0.5

         =180.5=36 rad/s



Q 2 :

A small block is shot into each of the four tracks as shown below. Each of the tracks rises to the same height. The speed with which the block enters the track is the same in all cases. At the highest point of the track, the normal reaction is maximum in                    [2001]

  • [IMAGE 64]

     

  • [IMAGE 65]

     

  • [IMAGE 66]

     

  • [IMAGE 67]

     

(1)

According to question, the speed with which the block enters the track is the same in all the tracks and the block rises to the same height, so from the law of conservation of energy, speed of the block at the highest point will be same in all four cases.

Let the velocity at the highest point be v.

[IMAGE 68]

(N+mg) provides the centripetal force mv2R to the body

              N+mg=mv2R

or         N=mv2R-mg

R (the radius of curvature) in the first case is minimum.

Hence, normal reaction N will be maximum in the first case.



Q 3 :

A thin circular coin of mass 5 gm and radius 43 cm is initially in a horizontal xy-plane. The coin is tossed vertically up (+z direction) by applying an impulse of  π2×10-2 N - s at a distance 23 cm from its center. The coin spins about its diameter and moves along the +z direction. By the time the coin reaches back to its initial position, it completes n rotations. The value of n is ________.

[Given: The acceleration due to gravity g=10ms-2]                [2023]

[IMAGE 69]



(30)

From impulse--momentum theorem,

J=MVCM    V=JM=π/2100×51000=2π m/s

Total time taken, t=2vg

=2×2πg=2×2π10=2π5s

By angular impulse--momentum theorem,

J×R2=ICω=[14MR2]ω

 ω=J×R2MR24=J×2MR

=π/2100×251000×43×1100=2×752π rad/s

 θ=2πn=ωt    n=ωt2π

 n=2×752π×2π52π=30



Q 4 :

A wire, which passes through the hole in a small bead, is bent in the form of a quarter of a circle. The wire is fixed vertically on ground as shown in the figure. The bead is released from near the top of the wire and it slides along the wire without friction. As the bead moves from A to B, the force it applies on the wire is            [2014]

[IMAGE 70]

  • always radially outwards

     

  • always radially inwards

     

  • radially outwards initially and radially inwards later

     

  • radially inwards initially and radially outwards later

     

(4)

[IMAGE 71]

Suppose 'N' is acting radially outward.

Then, mgcosθ-N=mv2R

N=mgcosθ-mv2R                     ...(i)

And by energy conservation,

12mv2=mg[R-Rcosθ]

 v2R=2g(1-cosθ)

Putting this value of v2R in eqn. (i),

N=mgcosθ-m[2g-2gcosθ]

N=mgcosθ-2mg+2mgcosθ

N=3mgcosθ-2mgN=mg(3cosθ-2)

Clearly when cosθ>23, N is positive and acts radially outward.

So, force on wire is inward and if cosθ<23, N acts radially inward.

So, force on wire is outward.