Q 1 :

A block (B) is attached to two unstretched springs S1 and S2 with spring constants k and 4k, respectively (see fig. I). The other ends are attached to identical supports M1 and M2 not attached to the walls. The springs and supports have negligible mass. There is no friction anywhere. The block B is displaced towards wall 1 by a small distance x (figure II) and released. The block returns and moves a maximum distance y towards wall 2. Displacements x and y are measured with respect to the equilibrium position of the block B. The ratio y/x is                              [2008]

[IMAGE 111]

  • 4

     

  • 2

     

  • 1/2

     

  • 1/4

     

(3)

Here when the block B is displaced towards wall 1, only spring S1 is compressed and S2 is in its natural state as the other end of S2 is free.

Therefore the energy stored in the system =12k1x2

When the block is released, it will come back to the equilibrium position, gain momentum, overshoot the equilibrium position and move towards wall 2. As this happens, the spring S1 comes to its natural length and S2 gets compressed. The P.E. stored in the spring S1 gets stored as the P.E. of spring S2 when the block B reaches its extreme position after compressing S2 by y. It is because no friction anywhere.

So, energy is conserved

 12k1x2=12k2y212kx2=12×4ky2

x2=4y2   yx=12



Q 2 :

A particle is acted by a force F=kx, where k is a +ve constant. Its potential energy at x=0 is zero. Which curve correctly represents the variation of potential energy of the block with respect to x                                   [2004]

  • [IMAGE 112]

     

  • [IMAGE 113]

     

  • [IMAGE 114]

     

  • [IMAGE 115]

     

(2)

For conservative forces ΔU=-W

ΔU=-0xFdx   or   ΔU=-0xkxdx

U(x)-U(0)=-kx22         (U(0)=0)

 U(x)=-kx22     x2=-2Uxk

It represents a parabola below the x-axis symmetrical.



Q 3 :

An ideal spring with spring-constant k is hung from the ceiling and a block of mass M is attached to its lower end. The mass is released with the spring initially unstretched. Then the maximum extension in the spring is                    [2002]

  • 4Mgk

     

  • 2Mgk

     

  • Mgk

     

  • Mg2k

     

(2)

Let x be the maximum extension of the string. Here mechanical energy is conserved, so decrease in the gravitational potential energy of spring mass system (Mgx)

= gain in spring elastic potential energy (12kx2)

Mgx=12kx2    x=2Mgk



Q 4 :

A particle, which is constrained to move along the x-axis, is subjected to a force in the same direction which varies with the distance x of the particle from the origin as F(x)=-kx+ax3. Here k and a are positive constants. For x0, the functional form of the potential energy U(x) of the particle is                     [2002]

  • [IMAGE 116]

     

  • [IMAGE 117]

     

  • [IMAGE 118]

     

  • [IMAGE 119]

     

(4)

 



Q 5 :

Consider an elliptical shaped rail PQ in the vertical plane with OP=3 m and OQ=4 m. A block of mass 1 kg is pulled along the rail from P to Q with a force of 18 N, which is always parallel to line PQ (see the figure given). Assuming no frictional losses, the kinetic energy of the block when it reaches Q is (n×10) joules. The value of n is (take acceleration due to gravity =10 ms-2)                     [2014]

[IMAGE 120]



(5)

Work done = Increase in P.E. + gain in K.E.

F×d=mgh+gain in K.E.

18×5=1×10×4+gain in K.E.

 Gain in K.E.=50 J=10n  n=5



Q 6 :

A block of mass 0.18 kg is attached to a spring of force constant 2 N/m. The coefficient of friction between the block and the floor is 0.1. Initially the block is at rest and the spring is unstretched. An impulse is given to the block as shown in the figure. The block slides a distance of 0.06 m and comes to rest for the first time. The initial velocity of the block in m/s is V = N10. Then N is                           [2011]

[IMAGE 121]



(4)

Here, loss in K.E. of the block = gain in P.E. of the spring + work done against friction

12mv2=12kx2+μmgx   v=2μmgx+kx2m

v=2×0.1×0.18×10×0.6+2×0.6×0.60.18

 v=410=N10        N=4



Q 7 :

A student skates up a ramp that makes an angle 30° with the horizontal. He/she starts (as shown in the figure) at the bottom of the ramp with speed v0 and wants to turn around over a semicircular path xyz of radius R during which he/she reaches a maximum height h (at point y) from the ground as shown in the figure. Assume that the energy loss is negligible and the force required for this turn at the highest point is provided by his/her weight only. Then (g is the acceleration due to gravity)      [2020]

[IMAGE 122]

  • v02-2gh=12gR

     

  • v02-2gh=32gR

     

  • the centripetal force required at points x and z is zero

     

  • the centripetal force required is maximum at points x and z

     

Select one or more options

(1, 4)

At point Y the centripetal force provided by the component of weight mg

 mgsin30°=mv2R

 v2=gR2

Now by the energy conservation between bottom point and point Y

[IMAGE 123]

12mv02=mgh+12mv2

 v2=v02-2gh              ...(i)

 From eq. (i)  

gR2=v02-2gh

Hence option (1) is correct.

At point x and z of circular path, the points are at same height but less than h. So the velocity is more than at point y.

So required centripetal force =mv2r is maximum at points x and y.



Q 8 :

A particle of mass m is initially at rest at the origin. It is subjected to a force and starts moving along the x-axis. Its kinetic energy K changes with time as dKdt=γt, where γ is a positive constant of appropriate dimensions. Which of the following statements is (are) true?            [2018]

  • The force applied on the particle is constant

     

  • The speed of the particle is proportional to time

     

  • The distance of the particle from the origin increases linearly with time

     

  • The force is conservative

     

Select one or more options

(1, 2, 4)

Gdkdt=γt  and  k=12mV2               ddt(12mV2)=γt

m2×2VdVdt=γt             mVdVdt=γt

 m0VVdV=γ0ttdt            mV22=γt22

 V=γm×t  i.e., Vt;    V=dsdt=γmt     s=γm·t22

So V is proportional to 't' and distance cannot be proportional to 't'.

Now F=ma=mdVdt=mddt(γm×t)=mγm=γm=constant

Since force applied is constant and displacement between any two points on x-axis will also be constant, thus work done will be independent of path. Hence force is conservative in nature.



Q 9 :

A small ball starts moving from A over a fixed track as shown in the figure. Surface AB has friction. From A to B the ball rolls without slipping. Surface BC is frictionless. KA, KB and KC are kinetic energies of the ball at A, B and C, respectively. Then              [2006]

[IMAGE 124]

  • hA>hC; KB>KC

     

  • hA>hC; KC>KA

     

  • hA=hC; KB=KC

     

  • hA<hC; KB>KC

     

Select one or more options

(1, 2, 4)

From figure given in question,

Potential energy of the ball at point A =mghA

Potential energy of the ball at point B = 0

Potential energy of the ball at point C =mghC

Total energy at point A, EA=KA+mghA

Total energy at point B, EB=KB

Total energy at point C, EC=KC+mghC

As body rolls between A and B and between B and C there is no friction. So energy should be conserved here.

By law of conservation of energy

EA=EB=EC

As EA=EC

KA+mghA=KC+mghC

So, if hA>hCKA<KC. So option (2) is correct.

If hA<hCKA>KC

Doesn't matter if hA>hC or hA<hC, we will always have KB>KC

because EA=EB=EC. So option (1) and (4) is also correct.



Q 10 :

A small block of mass 1 kg is released from rest at the top of a rough track. The track is a circular arc of radius 40 m. The block slides along the track without toppling and a frictional force acts on it in the direction opposite to the instantaneous velocity. The work done in overcoming the friction up to the point Q, as shown in the figure below, is 150 J.

(Take the acceleration due to gravity, g=10 ms-2)                                    [2013]

[IMAGE 125]

Q.   The magnitude of the normal reaction that acts on the block at the point Q is

  • 7.5 N

     

  • 8.6 N

     

  • 11.5 N

     

  • 22.5 N

     

(1)

[IMAGE 126]

As Wall forces=ΔK Wmg+Wfr=12mv2-0

mgh-150=12mv2

mgRsin30°-150=12mv21×10×40×12-150=v22

v=10 m/s

N-mgcosθ will provide required centripetal force

N-mgcosθ=mv2R

N=mgcosθ+mv2R

=1×10×12+1×(10)240=7.5 N



Q 11 :

A small block of mass 1 kg is released from rest at the top of a rough track. The track is a circular arc of radius 40 m. The block slides along the track without toppling and a frictional force acts on it in the direction opposite to the instantaneous velocity. The work done in overcoming the friction up to the point Q, as shown in the figure below, is 150 J.

(Take the acceleration due to gravity, g=10 ms-2)                      [2013]

[IMAGE 127]

Q.  The speed of the block when it reaches the point Q is

  • 5 ms-1

     

  • 10 ms-1

     

  • 103 ms-1

     

  • 20 ms-1

     

(2)

As discussed earlier, we get v=10 m/s.



Q 12 :

STATEMENT–1: A block of mass m starts moving on a rough horizontal surface with a velocity v. It stops due to friction between the block and the surface after moving through a certain distance. The surface is now tilted to an angle of 30° with the horizontal and the same block is made to go up on the surface with the same initial velocity v. The decrease in the mechanical energy in the second situation is smaller than that in the first situation.

STATEMENT–2: The coefficient of friction between the block and the surface decreases with the increase in the angle of inclination.              [2007]

  • Statement–1 is True, Statement–2 is True; Statement–2 is a correct explanation for Statement–1

     

  • Statement–1 is True, Statement–2 is True; Statement–2 is NOT a correct explanation for Statement–1

     

  • Statement–1 is True, Statement–2 is False

     

  • Statement–1 is False, Statement–2 is True

     

(3)

In the first case the mechanical energy is completely converted into heat because of friction, i.e., decrease in mechanical energy =12mv2

While in second case, a part of mechanical energy is converted into heat due to friction but another part of mechanical energy is retained in the form of potential energy of the block, i.e., Decrease in mechanical energy =12mv2-mgh

Therefore statement 1 is correct.

Statement 2 is wrong. The coefficient of friction between the block and the surface does not depend on the angle of inclination.