#### Chapters

Chapter 2: Units and Measurements

Chapter 3: Motion in a Straight Line

Chapter 4: Motion in a Plane

Chapter 5: Laws of Motion

Chapter 6: Work, Energy and Power

Chapter 7: System of Particles and Rotational Motion

Chapter 8: Gravitation

Chapter 9: Mechanical Properties of Solids

Chapter 10: Mechanical Properties of Fluids

Chapter 11: Thermal Properties of Matter

Chapter 12: Thermodynamics

Chapter 13: Kinetic Theory

Chapter 14: Oscillations

Chapter 15: Waves

## Chapter 14: Oscillations

#### NCERT solutions for Class 11 Physics Textbook Chapter 14 Oscillations [Pages 357 - 361]

Which of the following examples represent periodic motion?

(a) A swimmer completing one (return) trip from one bank of a river to the other and back.

(b) A freely suspended bar magnet displaced from its N-S direction and released.

(c) A hydrogen molecule rotating about its center of mass.

(d) An arrow released from a bow.

Which of the following examples represent (nearly) simple harmonic motion and which represent periodic but not simple harmonic motion?

(a) the rotation of the earth about its axis.

(b) a motion of an oscillating mercury column in a U-tube.

(c) the motion of a ball bearing inside a smooth curved bowl, when released from a point slightly above the lowermost point.

(d) general vibrations of a polyatomic molecule about its equilibrium position.

Figure depicts four *x-t *plots for linear motion of a particle. Which of the plots represent periodic motion? What is the period of motion (in case of periodic motion)?

Which of the following functions of time represent (a) simple harmonic, (b) periodic but not simple harmonic, and (c) non-periodic motion? Give period for each case of periodic motion (ω is any positive constant):

a) sin *ω**t *– cos *ω**t*

(b) sin^{3} *ω**t*

(c) 3 cos (π/4 – 2*ω**t*)

(d) cos ω*t *+ cos 3*ω**t** *+ cos 5*ω**t*

(e) exp (–*ω*^{2}*t*^{2})

(f) 1 + *ω**t *+ *ω*^{2}*t*^{2}

A particle is in linear simple harmonic motion between two points, A and B, 10 cm apart. Take the direction from A to B as the positive direction and give the signs of velocity, acceleration and force on the particle when it is

(a) at the end A,

(b) at the end B,

(c) at the mid-point of AB going towards A,

(d) at 2 cm away from B going towards A,

(e) at 3 cm away from A going towards B, and

(f) at 4 cm away from B going towards A.

Which of the following relationships between the acceleration a and the displacement x of a particle involve simple harmonic motion?

(a) a = 0.7x

(b) a = –200x^{2}

(c) a = –10x

(d) a = 100x^{3}

The motion of a particle executing simple harmonic motion is described by the displacement function,

*x* (*t*) = *A *cos (ω*t *+ φ).

If the initial (*t *= 0) position of the particle is 1 cm and its initial velocity is ω cm/s, what are its amplitude and initial phase angle? The angular frequency of the particle is π s^{–1}. If instead of the cosine function, we choose the sine function to describe the SHM: *x = B sin *(*ωt *+ α), what are the amplitude and initial phase of the particle with the above initial conditions.

A spring balance has a scale that reads from 0 to 50 kg. The length of the scale is 20 cm. A body suspended from this balance, when displaced and released, oscillates with a period of 0.6 s. What is the weight of the body?

A spring having with a spring constant 1200 N m^{–1} is mounted on a horizontal table as shown in Fig. A mass of 3 kg is attached to the free end of the spring. The mass is then pulled sideways to a distance of 2.0 cm and released.

Determine (i) the frequency of oscillations, (ii) maximum acceleration of the mass, and (iii) the maximum speed of the mass.

let us take the position of mass when the spring is unstretched as *x = *0, and the direction from left to right as the positive direction of the *x*-axis. Give *x *as a function of time t for the oscillating mass if at the moment we start the stopwatch (*t *= 0), the mass is

(a) at the mean position,

(b) at the maximum stretched position, and

(c) at the maximum compressed position.

In what way do these functions for SHM differ from each other, in frequency, in amplitude or the initial phase?

Figures correspond to two circular motions. The radius of the circle, the period of revolution, the initial position, and the sense of revolution (i.e. clockwise or anti-clockwise) are indicated on each figure

Obtain the corresponding simple harmonic motions of the *x*-projection of the radius vector of the revolving particle P, in each case.

Plot the corresponding reference circle for each of the following simple harmonic motions. Indicate the initial (*t *= 0) position of the particle, the radius of the circle, and the angular speed of the rotating particle. For simplicity, the sense of rotation may be fixed to be anticlockwise in every case: (*x *is in cm and *t *is in *s*).

(a) *x *= –2 sin (3*t *+ π/3)

(b) *x *= cos (π/6 – *t*)

(c) *x *= 3 sin (2π*t *+ π/4)

(d) *x *= 2 cos π*t*

Figure (a) shows a spring of force constant *k *clamped rigidly at one end and a mass *m *attached to its free end. A force *F* applied at the free end stretches the spring. Figure (b) shows the same spring with both ends free and attached to a mass *m*at either end. Each end of the spring in Fig. (b) is stretched by the same force *F*.

(a) What is the maximum extension of the spring in the two cases?

(b) If the mass in Fig. (a) and the two masses in Fig. (b) are released, what is the period of oscillation in each case?

The piston in the cylinder head of a locomotive has a stroke (twice the amplitude) of 1.0 m. If the piston moves with simple harmonic motion with an angular frequency of 200 rad/min, what is its maximum speed?

The acceleration due to gravity on the surface of moon is 1.7 ms^{–2}. What is the time period of a simple pendulum on the surface of moon if its time period on the surface of earth is 3.5 s? (*g *on the surface of earth is 9.8 ms^{–2})

Answer the following questions:

A time period of a particle in SHM depends on the force constant *k *and mass *m *of the particle: `T = 2pi sqrt(m/k)` A simple pendulum executes SHM approximately. Why then is the time

Answer the following questions:

The motion of a simple pendulum is approximately simple harmonic for small angle oscillations. For larger angles of oscillation, a more involved analysis shows that *T *is greater than `2pisqrt(1/g)` Think of a qualitative argument to appreciate this result.

Answer the following questions:

A man with a wristwatch on his hand falls from the top of a tower. Does the watch give correct time during the free fall?

Answer the following questions:

What is the frequency of oscillation of a simple pendulum mounted in a cabin that is freely falling under gravity?

A simple pendulum of length *l *and having a bob of mass *M *is suspended in a car. The car is moving on a circular track of radius *R *with a uniform speed *v*. If the pendulum makes small oscillations in a radial direction about its equilibrium position, what will be its time period?

The cylindrical piece of the cork of density of base area *A *and height *h *floats in a liquid of density `rho_1`. The cork is depressed slightly and then released. Show that the cork oscillates up and down simple harmonically with a period

`T = 2pi sqrt((hrho)/(rho_1g)`

where *ρ* is the density of cork. (Ignore damping due to viscosity of the liquid).

One end of a U-tube containing mercury is connected to a suction pump and the other end to the atmosphere. A small pressure difference is maintained between the two columns. Show that, when the suction pump is removed, the column of mercury in the U-tube executes simple harmonic motion.

An air chamber of volume V has a neck area of cross section a into which a ball of mass m just fits and can move up and down without any friction (Fig.14.33). Show that when the ball is pressed down a little and released, it executes SHM. Obtain an expression for the time period of oscillations assuming pressure-volume variations of air to be isothermal

You are riding in an automobile of mass 3000 kg. Assuming that you are examining the oscillation characteristics of its suspension system. The suspension sags 15 cm when the entire automobile is placed on it. Also, the amplitude of oscillation decreases by 50% during one complete oscillation. Estimate the values of (a) the spring constant *k *and (b) the damping constant *b *for the spring and shock absorber system of one wheel, assuming that each wheel supports 750 kg.

Show that for a particle in linear SHM the average kinetic energy over a period of oscillation equals the average potential energy over the same period.

A circular disc of mass 10 kg is suspended by a wire attached to its centre. The wire is twisted by rotating the disc and released. The period of torsional oscillations is found to be 1.5 s. The radius of the disc is 15 cm. Determine the torsional spring constant of the wire. (Torsional spring constant α is defined by the relation *J *= –α *θ,* where *J *is the restoring couple and *θ* the angle of twist).

A body describes simple harmonic motion with an amplitude of 5 cm and a period of 0.2 s. Find the acceleration and velocity of the body when the displacement is (a) 5 cm, (b) 3 cm, (c) 0 cm.

A mass attached to a spring is free to oscillate, with angular velocity ω, in a horizontal plane without friction or damping. It is pulled to a distance *x*_{0} and pushed towards the centre with a velocity *v*_{0} at time *t *= 0. Determine the amplitude of the resulting oscillations in terms of the parameters ω, *x*_{0} and *v*_{0}. [Hint: Start with the equation *x *= *a*cos (*ω**t**+θ*) and note that the initial velocity is negative.]

## Chapter 14: Oscillations

## NCERT solutions for Class 11 Physics Textbook chapter 14 - Oscillations

NCERT solutions for Class 11 Physics Textbook chapter 14 (Oscillations) include all questions with solution and detail explanation. This will clear students doubts about any question and improve application skills while preparing for board exams. The detailed, step-by-step solutions will help you understand the concepts better and clear your confusions, if any. Shaalaa.com has the CBSE Class 11 Physics Textbook solutions in a manner that help students grasp basic concepts better and faster.

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Concepts covered in Class 11 Physics Textbook chapter 14 Oscillations are Force Law for Simple Harmonic Motion, Energy in Simple Harmonic Motion, Some Systems Executing Simple Harmonic Motion, Damped Simple Harmonic Motion, Forced Oscillations and Resonance, Displacement as a Function of Time, Periodic Functions, Oscillations - Frequency, Periodic and Oscillatory Motions, Simple Harmonic Motion, Simple Harmonic Motion and Uniform Circular Motion, Velocity and Acceleration in Simple Harmonic Motion.

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