A block is attached to two unstretched springs and with spring constants and , respectively (see fig. I). The other ends are attached to identical supports and not attached to the walls. The springs and supports have negligible mass. There is no friction anywhere. The block is displaced towards wall 1 by a small distance (figure II) and released. The block returns and moves a maximum distance towards wall 2. Displacements and are measured with respect to the equilibrium position of the block . The ratio is [2008]
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4
2
1/2
1/4
(3)
Here when the block B is displaced towards wall 1, only spring is compressed and is in its natural state as the other end of is free.
Therefore the energy stored in the system
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 comes to its natural length and gets compressed. The P.E. stored in the spring gets stored as the P.E. of spring when the block reaches its extreme position after compressing by . It is because no friction anywhere.
So, energy is conserved
A particle is acted by a force , where is a +ve constant. Its potential energy at is zero. Which curve correctly represents the variation of potential energy of the block with respect to [2004]
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(2)
It represents a parabola below the -axis symmetrical.
An ideal spring with spring-constant is hung from the ceiling and a block of mass is attached to its lower end. The mass is released with the spring initially unstretched. Then the maximum extension in the spring is [2002]
(2)
Let be the maximum extension of the string. Here mechanical energy is conserved, so decrease in the gravitational potential energy of spring mass system
= gain in spring elastic potential energy
A particle, which is constrained to move along the -axis, is subjected to a force in the same direction which varies with the distance of the particle from the origin as Here and are positive constants. For , the functional form of the potential energy of the particle is [2002]
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Consider an elliptical shaped rail in the vertical plane with and . 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 joules. The value of is (take acceleration due to gravity ) [2014]
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(5)
Work done = Increase in P.E. + gain in K.E.
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 = . Then N is [2011]
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(4)
Here, loss in K.E. of the block = gain in P.E. of the spring + work done against friction
A student skates up a ramp that makes an angle with the horizontal. He/she starts (as shown in the figure) at the bottom of the ramp with speed and wants to turn around over a semicircular path of radius during which he/she reaches a maximum height (at point ) 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 ( is the acceleration due to gravity) [2020]
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the centripetal force required at points and is zero
the centripetal force required is maximum at points and
Select one or more options
(1, 4)
At point Y the centripetal force provided by the component of weight mg
Now by the energy conservation between bottom point and point Y
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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 is maximum at points x and y.
A particle of mass is initially at rest at the origin. It is subjected to a force and starts moving along the -axis. Its kinetic energy changes with time as , where 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)
So is proportional to and distance cannot be proportional to .
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.
A small ball starts moving from over a fixed track as shown in the figure. Surface has friction. From to the ball rolls without slipping. Surface is frictionless. , and are kinetic energies of the ball at A, B and C, respectively. Then [2006]
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Select one or more options
(1, 2, 4)
From figure given in question,
Potential energy of the ball at point A
Potential energy of the ball at point B = 0
Potential energy of the ball at point C
Total energy at point A,
Total energy at point B,
Total energy at point C,
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
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, ) [2013]
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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)
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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, ) [2013]
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Q. The speed of the block when it reaches the point Q is
(2)
As discussed earlier, we get
STATEMENT–1: A block of mass starts moving on a rough horizontal surface with a velocity . 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 with the horizontal and the same block is made to go up on the surface with the same initial velocity . 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
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
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.