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      Class 11 PHYSICS – JEE

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      • Class 11
      • Class 11 PHYSICS – JEE
      CoursesClass 11PhysicsClass 11 PHYSICS – JEE
      • 1.Basic Maths (1) : Vectors
        7
        • Lecture1.1
          Vector and Scalar, Representation of Vectors, Need for Co-ordinate System, Distance & Displacement 39 min
        • Lecture1.2
          Mathematics of Vectors, Triangle Law and Parallelogram Law 01 hour
        • Lecture1.3
          Addition More than Two Vectors, Subtraction of Vectors- Displacement vector 28 min
        • Lecture1.4
          Elementary Maths 14 min
        • Lecture1.5
          Unit Vectors, Special Unit Vectors, Resolution of Vectors 49 min
        • Lecture1.6
          Addition & Subtract using Unit Vectors, 3 D Vectors, Product of Vectors 54 min
        • Lecture1.7
          Chapter Notes – Basic Maths (1) : Vectors
      • 2.Basic Maths (2) : Calculus
        4
        • Lecture2.1
          Delta, Concept of Infinity, Time Instant Interval, Rate of Change, Position and Velocity 40 min
        • Lecture2.2
          Fundamental Idea of Differentiation- Constant Multiplication Rule, Sum/Difference Rule 29 min
        • Lecture2.3
          Trigonometric functions, Log function, Product Rule, Quotient Rule, Chain Rule 25 min
        • Lecture2.4
          Integration- Formulas of Integration, Use of Integration 45 min
      • 3.Unit and Measurement
        13
        • Lecture3.1
          Unit, History of Unit of Length-Metre, Properties of a Good Unit 21 min
        • Lecture3.2
          Concept of Derived Units, Fundamental Physics Quantities and Prefix of Units 38 min
        • Lecture3.3
          Unit-less Derived Quantities, Supplementary Quantities, Systems of Unit, Unit Conversion 39 min
        • Lecture3.4
          Dimensional Analysis, Dimension and Unit, Dimensionless Quantities 32 min
        • Lecture3.5
          Principle of Homogeneity 34 min
        • Lecture3.6
          Dimensionally Correct/Incorrect Equations, Use of Dimensional Analysis 41 min
        • Lecture3.7
          More Units of Length and Measurement of Length 47 min
        • Lecture3.8
          Errors and Their Reasons 36 min
        • Lecture3.9
          Combination of Errors 42 min
        • Lecture3.10
          Round Off, Significant Figures, Exponent Form of Numbers/Scientific Notation 27 min
        • Lecture3.11
          Chapter Notes – Unit and Measurement
        • Lecture3.12
          NCERT Solutions – Unit and Measurement
        • Lecture3.13
          Revision Notes – Unit and Measurement
      • 4.Motion (1) : Straight Line Motion
        10
        • Lecture4.1
          Meaning of Dimension; Position; Distance & Displacement 25 min
        • Lecture4.2
          Average Speed & Velocity; Instantaneous Speed & Velocity 31 min
        • Lecture4.3
          Photo Diagram; Acceleration- Direction of acceleration, Conceptual Examples 22 min
        • Lecture4.4
          Constant Acceleration; Equations of constant acceleration 43 min
        • Lecture4.5
          Average Velocity Examples and Concepts; Reaction Time 19 min
        • Lecture4.6
          Free Fall under Gravity 30 min
        • Lecture4.7
          Variable Acceleration; Derivation of Constant Acceleration Equations 48 min
        • Lecture4.8
          Chapter Notes – Motion (1) : Straight Line Motion
        • Lecture4.9
          NCERT Solutions – Straight Line Motion
        • Lecture4.10
          Revision Notes Straight Line Motion
      • 5.Motion (2) : Graphs
        3
        • Lecture5.1
          Tangent & Chord; Slope of Line- Chord & Tangent; Meaning of x/t graph, v/t graph, a/t graph 59 min
        • Lecture5.2
          Graph Conversion 51 min
        • Lecture5.3
          Area Under Curve 22 min
      • 6.Motion (3) : Two Dimensional Motion
        6
        • Lecture6.1
          Projectile on Level Ground 32 min
        • Lecture6.2
          Terms Related to Projectile on Level Ground 31 min
        • Lecture6.3
          Not Level to Level Projectile, Problem Solving, Dot Product 34 min
        • Lecture6.4
          Equation of Trajectory and Some Miscellaneous Questions 35 min
        • Lecture6.5
          Projectile on Inclined Plane 39 min
        • Lecture6.6
          Collision of Projectile and Avg. Acceleration in 2D Motion 16 min
      • 7.Motion (4) : Relative Motion
        7
        • Lecture7.1
          Reference Frame and Distance of Closest Approach 45 min
        • Lecture7.2
          Relative Motion in 2D 26 min
        • Lecture7.3
          Free Fall & Relative Motion 26 min
        • Lecture7.4
          Throwing Object from Moving Body 32 min
        • Lecture7.5
          Rain Problem (theory)- and Wind in Rain Problem 32 min
        • Lecture7.6
          River Based Problem 26 min
        • Lecture7.7
          Crossing River by Shortest Distance- Least Time to Cross River; Wind Problems; Relative Approach 27 min
      • 8.Newton's Laws of Motion
        8
        • Lecture8.1
          Force and Newton’s Laws 33 min
        • Lecture8.2
          Normal Reaction, Free Body Diagram(F.B.D), Normal on circular bodies, Mass and Weight 57 min
        • Lecture8.3
          Tension Force(Ideal Pulley, Clamp Force), Internal & External Force, Heavy Rope 01 hour
        • Lecture8.4
          Spring Force(Sudden Change, Series and Parallel Cutting of Spring) 01 hour
        • Lecture8.5
          Inertia and Non-Inertial Frames(Pseudo Force), Action-Reactin Pair, Monkey Problem 49 min
        • Lecture8.6
          Chapter Notes – Newton’s Laws of Motion
        • Lecture8.7
          NCERT Solutions – Laws of Motion
        • Lecture8.8
          Revision Notes Laws of Motion
      • 9.Constrain Motion
        3
        • Lecture9.1
          Force of mass-less body; Constrain Motion- Pulley Constrain 1 01 hour
        • Lecture9.2
          Pulley constrain 2, Alternate Method; Wedge Constrain- Proof 49 min
        • Lecture9.3
          Relative Constrain 01 hour
      • 10.Friction
        6
        • Lecture10.1
          Kinetic friction Theory- Theory, Angle of friction 32 min
        • Lecture10.2
          Static Friction Theory- Based on Example 2, Direction of friction Theory 01 min
        • Lecture10.3
          Some Advanced Examples 18 min
        • Lecture10.4
          Block Over Block Theory 01 hour
        • Lecture10.5
          Conveyor belt, Static and kinetic co-eff. of friction, Friction on wheels, Theoretical examples 27 min
        • Lecture10.6
          Chapter Notes – Friction
      • 11.Circular Motion
        6
        • Lecture11.1
          Ex. on Average Acc. and Angular Variables Theory and Ref. Frame 52 min
        • Lecture11.2
          Uniform Circular Motion and Centripetal Force 40 min
        • Lecture11.3
          Non-Uniform Center of Mass – Theory by Ex 2; Friction 01 hour
        • Lecture11.4
          Centrifugal Force and Banking of Roads 01 hour
        • Lecture11.5
          Radius of Curvature- Radius of Curvature; Axial Vector; Well of Death 34 min
        • Lecture11.6
          Chapter Notes – Circular Motion
      • 12.Work Energy Power
        15
        • Lecture12.1
          Work & its calculation and Work-done on curved path 31 min
        • Lecture12.2
          Work-done by Different Forces 01 hour
        • Lecture12.3
          Work Energy Theorem and W.E. th in Non-inertial frame, W.E. th and Time 23 min
        • Lecture12.4
          Work Energy Theorem for System 55 min
        • Lecture12.5
          Energy and Different Forms of Energy-and Energy of Chain; Potential Energy & Reference Frame 28 min
        • Lecture12.6
          Potential Energy Curve and Power 01 hour
        • Lecture12.7
          Normal Reaction, Vertical Circular Motion, Motion in Co-Concentric Spheres 27 min
        • Lecture12.8
          Motion on Outer Surface of Sphere, Motion on Inner Surface of Fixed Sphere 59 min
        • Lecture12.9
          Motion on Rope, Motion on Rod 32 min
        • Lecture12.10
          VCM – 1 31 min
        • Lecture12.11
          VCM – 2 01 hour
        • Lecture12.12
          VCM – 3 22 min
        • Lecture12.13
          Chapter Notes – Work Energy Power
        • Lecture12.14
          NCERT Solutions – Work Energy Power
        • Lecture12.15
          Revision Notes Work Energy Power
      • 13.Momentum
        9
        • Lecture13.1
          Introduction and Conservation of Momentum 35 min
        • Lecture13.2
          Impulsive Force – Characteristics of Impulsive Force 30 min
        • Lecture13.3
          Momentum Conservation in Presence of External Force – Two Steps Problems 41 min
        • Lecture13.4
          Questions Involving Momentum & Work Energy Theorem 27 min
        • Lecture13.5
          Collision – Head – on Collision and Special Cases of Head – on Collision 39 min
        • Lecture13.6
          Oblique Collision 24 min
        • Lecture13.7
          Collision of Ball with Flat Surface 38 min
        • Lecture13.8
          Impulse and Average Force 58 min
        • Lecture13.9
          Advanced Questions 50 min
      • 14.Center of Mass
        5
        • Lecture14.1
          Center of Mass (CM) Frame and Kinetic Energy in C – Frame 29 min
        • Lecture14.2
          Finding Center of Mass by Replacement Method and Finding CM of Plate with Hole 36 min
        • Lecture14.3
          Finding CM by Integration and CM of Some Standard Objects 57 min
        • Lecture14.4
          Motion of CM; Newton’s 2nd Law for CM; CM in Circular Motion 41 min
        • Lecture14.5
          Revision Notes Center of Mass
      • 15.Rotational Motion
        14
        • Lecture15.1
          Rigid Body – Motion of Rigid Body; Axis of Rotation 14 min
        • Lecture15.2
          Vector Product/ Cross Product; Torque 44 min
        • Lecture15.3
          Couple and Principle of Moments 48 min
        • Lecture15.4
          Pseudo Force and Toppling – Overturning of Car 01 hour
        • Lecture15.5
          Moment of Inertia 01 hour
        • Lecture15.6
          Parallel Axis Theorem; Perpendicular Axis Theorem; Quantitative Analysis; Radius of Gyra 01 hour
        • Lecture15.7
          Analogy b/w Transnational & Rotational Motion; Relation b/w Linear and Angular Velocity; Dynamics of Rotation 40 min
        • Lecture15.8
          Angular Momentum 30 min
        • Lecture15.9
          Angular Momentum of a Particle 32 min
        • Lecture15.10
          Rotational Collision 49 min
        • Lecture15.11
          Kinetic Energy, Work, Power; Potential Energy; Linear & Angular Acceleration; Hinge Force; Angular Impulse 02 hour
        • Lecture15.12
          Chapter Notes – Rotational Motion and Rolling Motion
        • Lecture15.13
          NCERT Solutions – Rotational Motion
        • Lecture15.14
          Revision Notes Rotational Motion
      • 16.Rolling Motion
        11
        • Lecture16.1
          Introduction to Rolling Motion 40 min
        • Lecture16.2
          Rolling Motion on Spool 24 min
        • Lecture16.3
          Friction 59 min
        • Lecture16.4
          Direction of Friction 01 hour
        • Lecture16.5
          Rolling on Moving Platform and Motion of Touching Spheres 44 min
        • Lecture16.6
          Rope Based Questions 55 min
        • Lecture16.7
          Work-done by Friction in Rolling Motion, Kinetic Energy in Transnational + Rotational Motion 29 min
        • Lecture16.8
          Angular Momentum in Rotation + Translation 01 hour
        • Lecture16.9
          Angular Collision 01 hour
        • Lecture16.10
          Instantaneous Axis of Rotation 50 min
        • Lecture16.11
          De-Lambart’s Theorem 50 min
      • 17.Gravitation
        8
        • Lecture17.1
          Gravitation force, Universal Law of Gravitation, Gravitational Force due to Hollow Sphere and Solid Sphere 35 min
        • Lecture17.2
          Acceleration due to Gravity and Rotation of Earth 42 min
        • Lecture17.3
          Potential Energy, Questions and Solutions 56 min
        • Lecture17.4
          Satellites, Circular Motion, Geostationary Satellites and Polar Satellites 42 min
        • Lecture17.5
          Polar Satellites, Weightlessness in Satellites, Trajectories and Kepler’s Laws 29 min
        • Lecture17.6
          Chapter Notes – Gravitation
        • Lecture17.7
          NCERT Solutions – Gravitation
        • Lecture17.8
          Revision Notes Gravitation
      • 18.Simple Harmonic Motion
        13
        • Lecture18.1
          Oscillatory Motion – Horizontal Spring Block System, Qualitative Analysis of Horizontal Spring System 33 min
        • Lecture18.2
          Quantitative Analysis of Horizontal Spring System; Frequency and Angular Frequency; Velocity and Acceleration; Mechanical Energy 47 min
        • Lecture18.3
          Relating Uniform Circular Motion and SHM and Phasor Diagram 30 min
        • Lecture18.4
          Equation of SHM and Problem Solving using Phasor Diagram 39 min
        • Lecture18.5
          Questions 40 min
        • Lecture18.6
          More Oscillating Systems – Vertical Spring Block System 41 min
        • Lecture18.7
          Angular Oscillations – Simple Pendulum 34 min
        • Lecture18.8
          Compound / Physical Pendulum, Torsional Pendulum, Equilibrium of Angular SHM; Differentiation by Chain Rule 38 min
        • Lecture18.9
          Energy Method to find Time Period 30 min
        • Lecture18.10
          Finding Amplitude of SHM 30 min
        • Lecture18.11
          Block Over Block and Elastic Rope 33 min
        • Lecture18.12
          Superposition of Horizontal SHMs and Perpendicular 30 min
        • Lecture18.13
          Damped Oscillations 28 min
      • 19.Waves (Part-1)
        11
        • Lecture19.1
          Wave, Plotting and Shifting of Curves, Meaning of y/t and y/x Graph, Wave is an Illusion!, 1D Wave on String 55 min
        • Lecture19.2
          Wave Equation, Analysis of Wave Equation and Wave Velocity 55 min
        • Lecture19.3
          Sinusoidal Wave (Harmonic Wave), Wave Equation for Sinusoidal Wave, Particle Velocity, Slope of Rope, Wave Velocity 01 hour
        • Lecture19.4
          Superposition of Waves 44 min
        • Lecture19.5
          Reflection of Waves 37 min
        • Lecture19.6
          Standing Waves 01 hour
        • Lecture19.7
          Tuning Fork, Sonometer and Equation of Standing Waves 54 min
        • Lecture19.8
          Energy in Waves 54 min
        • Lecture19.9
          Chapter Notes – Waves
        • Lecture19.10
          NCERT Solutions – Waves
        • Lecture19.11
          Revision Notes Waves
      • 20.Waves (Part-2)
        10
        • Lecture20.1
          Waves, Propagation of Sound Wave and Wave Equation 27 min
        • Lecture20.2
          Sound as a Pressure Wave 38 min
        • Lecture20.3
          Speed of Sound, Laplace Correction and Intensity of Sound Waves 59 min
        • Lecture20.4
          Spherical and Cylindrical Sound Waves 31 min
        • Lecture20.5
          Addition of Sin Functions, Interference of Sound Waves of Same Frequency, Interference of Coherent Sources 01 hour
        • Lecture20.6
          Quinke’s Apparatus 32 min
        • Lecture20.7
          Interference of Sound Waves of Slightly Different Frequencies (Beats) 39 min
        • Lecture20.8
          Reflection of Sound Waves, Standing Waves, End Correction 39 min
        • Lecture20.9
          Standing Waves in Terms of Pressure, Standing Waves on Rods, Kund’s Tube, Resonance Tube Experiment 49 min
        • Lecture20.10
          Doppler Effect, Reflection from Wall, Doppler Effect in 2 Dimension 01 hour
      • 21.Mechanical Properties of Solids
        6
        • Lecture21.1
          Rigid body,Strain, Stress,Hook’s Law 25 min
        • Lecture21.2
          Breaking Stress 26 min
        • Lecture21.3
          Shear Stress and Strain, Bulk Modulus, Elasticity and Plasticity, Stress-Strain Curve, Young’s Modulus 34 min
        • Lecture21.4
          Chapter Notes – Mechanical Properties of Solids
        • Lecture21.5
          NCERT Solutions – Mechanical Properties of Solids
        • Lecture21.6
          Revision Notes Mechanical Properties of Solids
      • 22.Thermal Expansion
        5
        • Lecture22.1
          Linear Expansion; Second’s Pendulum; Bimetallic Strip; Expansion of Hole; Thermal Stress 01 hour
        • Lecture22.2
          Areal/Superficial Expansion; Volume Expansion; Thermal Expansion of Liquid; Measurement of Temperature; Anomal 01 hour
        • Lecture22.3
          Arial/Superficial Expansion; Volume Expansion; Thermal Expansion of Liquid; Measurement of Temperature 38 min
        • Lecture22.4
          Chapter Notes – Thermal Expansion
        • Lecture22.5
          NCERT Solutions – Thermal Expansion
      • 23.Heat and Calorimetry
        2
        • Lecture23.1
          Internal Energy; Heat Energy; Thermal Equilibrium; Zeroth Law of Thermodynamics; Specific Heat Capacity; Latent Heat 48 min
        • Lecture23.2
          Mixing of Substances; Water Equivalent; Units; Calorimeter; Melting Point and Boiling Point; Sublimation 01 hour
      • 24.Heat Transfer
        6
        • Lecture24.1
          Conduction; Comparison between Charge Flow & Heat Flow 42 min
        • Lecture24.2
          Equivalent Thermal Conductivity; Heat Transfer and Calorimetry; Use of Integration; Length Variation 44 min
        • Lecture24.3
          Convection; Radiation, Black Body, Prevost Theory, Emissive Power & Emissivity, Kirchoff’s Law, Stefan – Boltzman Law 01 hour
        • Lecture24.4
          Newton’s Law of Cooling, Cooling Curve; Wien’s Displacement Law; Thermo Flask 48 min
        • Lecture24.5
          Chapter Notes – Heat Transfer
        • Lecture24.6
          Revision Notes Heat Transfer
      • 25.Kinetic Theory of Gases
        6
        • Lecture25.1
          Model of Gas,Postulates of Kinetic Theory of Gases, Ideal Gas, Mean free Path, Maxwell’s speed Distribution 37 min
        • Lecture25.2
          Volume, Pressure of Gases, Kinetic Energy, Temperature, Ideal Gas Equation 45 min
        • Lecture25.3
          Gas Laws, Internal energy of Gas, Degree of Freedom, Degree of Freedom of Mono-atomic and Diatomic Gas 56 min
        • Lecture25.4
          Chapter Notes – Kinetic Theory of Gases
        • Lecture25.5
          NCERT Solutions – Kinetic Theory of Gases
        • Lecture25.6
          Revision Notes Kinetic Theory of Gases
      • 26.Thermodynamics
        9
        • Lecture26.1
          State Equation; Thermodynamic Process; Process Equation & Graph; Work done by Gas 01 hour
        • Lecture26.2
          Heat – Work Equivalence; 1st Law of Thermodynamics; Adiabatic Process 57 min
        • Lecture26.3
          Workdone in Adiabatic Process; Specific Molar Heat Capacity 39 min
        • Lecture26.4
          Poly-tropic Process, Bulk Modulus; Free Expansion; Mixture of Gases 54 min
        • Lecture26.5
          Heat Engine, Refrigerator or Heat Pump, Energy Conservation, Kelvin-Plank Statement, Clausius Statement 01 hour
        • Lecture26.6
          Carnot Cycle, Reversible and Irreversible Process, Specific Heat Capacity of Solids and Water 01 hour
        • Lecture26.7
          Chapter Notes – Thermodynamics
        • Lecture26.8
          NCERT Solutions – Thermodynamics
        • Lecture26.9
          Revision Notes Thermodynamics
      • 27.Fluids
        14
        • Lecture27.1
          Introduction, Pressure of Liquid 47 min
        • Lecture27.2
          Manometer, Barometer 41 min
        • Lecture27.3
          Pascal Law, Hydraulic Lift 35 min
        • Lecture27.4
          Accelerated Liquid, Vertical and Horizontal Acceleration, Pressure Variation in Horizontally Accelerated Liquid 57 min
        • Lecture27.5
          Rotating Liquid, Rotating Liquid in U-Tube 28 min
        • Lecture27.6
          Archimedes’ Principle, Hollow Objects 59 min
        • Lecture27.7
          Apparent Weight, Variation of Liquid Force with Height 01 hour
        • Lecture27.8
          Multiple Liquids 34 min
        • Lecture27.9
          Center of Bouyancy 28 min
        • Lecture27.10
          Fluid Dynamics, Equation of Continuity 48 min
        • Lecture27.11
          Magnus Effect 37 min
        • Lecture27.12
          Venturimeter, Pitot Tube 27 min
        • Lecture27.13
          Questions and Solutions 31 min
        • Lecture27.14
          Chapter Notes – Fluids
      • 28.Surface Tension and Viscosity
        6
        • Lecture28.1
          Surface Tension, Surface Energy 52 min
        • Lecture28.2
          Force of Cohesion, Force of Adhesion, Angle of Contact, Radius of Meniscus, Capillary Rise 54 min
        • Lecture28.3
          Pressure Difference Across Meniscus, Variation of Surface tension with Temperature 27 min
        • Lecture28.4
          Viscous Force 35 min
        • Lecture28.5
          Terminal Velocity, Velocity Gradient, Renolds Number, Turbulent Flow, Streamline Flow 41 min
        • Lecture28.6
          Chapter Notes – Surface Tension and Viscosity

        NCERT Solutions – Waves

        15.1. A string of mass 2.50 kg is under a tension of 200 N. The length of the stretched string is 20.0 m. If the transverse jerk is struck at one end of the string, how long does the disturbance take to reach the other end? 

        Answer

        Mass of the string, M = 2.50 kg
        Tension in the string, T = 200 N
        Length of the string, l = 20.0 m
        Mass per unit length, µ = M/l = 2.50/20 = 0.125 kg m-1
        The velocity (v) of the transverse wave in the string is given by the relation:
        v = √t/µ
        = √200/0.125 = √1600 = 40 m/s
        ∴ Time taken by the disturbance to reach the other end, t = l/v = 20/40 = 0.5 s.

        15.2. A stone dropped from the top of a tower of height 300 m high splashes into the water of a pond near the base of the tower. When is the splash heard at the top given that the speed of sound in air is 340 m s–1? (g= 9.8 m s–2)

        Answer

        Height of the tower, s = 300 m
        Initial velocity of the stone, u = 0
        Acceleration, a = g = 9.8 m/s2
        Speed of sound in air = 340 m/s
        The time (t1) taken by the stone to strike the water in the pond can be calculated using the second equation of motion, as:
        s = ut1 + 1/2 gt12
        300 = 0 + 1/2 × 9.8 × t12
        ∴ t1 = √300 × 2/9.8  = 7.82 s
        Time taken by the sound to reach the top of the tower, t2 = 300/340 = 0.88 s
        Therefore, the time after which splash is heard,  t = t1 + t2
        = 7.82 + 0.88 = 8.7 s.

        15.3. A steel wire has a length of 12.0 m and a mass of 2.10 kg. What should be the tension in the wire so that speed of a transverse wave on the wire equals the speed of sound in dry air at 20 °C = 343 m s–1.

        Answer

        Length of the steel wire, l = 12 m
        Mass of the steel wire, m = 2.10 kg
        Velocity of the transverse wave, v = 343 m/s
        Mass per unit length, µ = m/l = 2.10/12 = 0.175 kg m-1
        For Tension T, velocity of the transverse wave can be obtained using the relation:
        v = √T/µ
        ∴ T = vu
        = (343)2 × 0.175 = 20588.575 ≈ 2.06 × 104 N.

        15.4. Use the formula v = √γP/ρ to explain why the speed of sound in air
        (a) is independent of pressure,
        (b) increases with temperature,
        (c) increases with humidity.

        Answer

        (a) Take the relation:
        v = √γP/ρ          ….(i)
        where,
        Density, ρ = Mass/Volume = M/V
        M = Molecular weight of the gas
        V = Volume of the gas
        Hence, equation (i) reduces to:
        v = √γPV/M       ….(ii)
        Now from the ideal gas equation for n = 1:
        PV = RT
        For constant T, PV = Constant
        Since both M and γ are constants, v = Constant
        Hence, at a constant temperature, the speed of sound in a gaseous medium is independent of the change in the pressure of the gas.

        (b) Take the relation:
        v = √γP/ρ          ….(i)
        For one mole of any ideal gas, the equation can be written as:
        PV = RT
        P = RT/V        ….(ii)
        Substituting equation (ii) in equation (i), we get:
        v = √γRT/Vρ  = √γRT/M  …..(iii)
        where,
        mass, M = ρV is a constant
        γ and R are also constants
        We conclude from equation (iii) that v ∝ √T
        Hence, the speed of sound in a gas is directly proportional to the square root of the temperature of the gaseous medium, i.e., the speed of the sound increases with an increase in the temperature of the gaseous medium and vice versa.

        (c) Let vm and vd be the speed of sound in moist air and dry air respectively.

        Let ρm and ρd be the densities of the moist air and dry air respectively.

        However, the presence of water vapour reduces the density of air, i.e.,
        ρd < ρm
        ∴ vm > vd

        Hence, the speed of sound in mois air is greater than it is in dry air. Thus, in gaseous medium, the speed of sound increases with humidity.

        15.5. You have learnt that a travelling wave in one dimension is represented by a function y = f (x, t)where x and t must appear in the combination x – v t or x + v t, i.e. y = f (x ± v t). Is the converse true? Examine if the following functions for y can possibly represent a travelling wave:

        (a) (x – vt)2
        (b) log [(x + vt) / x0]
        (c) 1 / (x + vt)

        Answer

        No, the converse is not true. The basic requirements for a wave function to represent a travelling wave is that for all values of x and t, wave function must have finite value.
        Out of the given functions for y, no one satisfies this condition. Therefore, none can represent a travelling wave.

        15.6. A bat emits ultrasonic sound of frequency 1000 kHz in air. If the sound meets a water surface, what is the wavelength of (a) the reflected sound, (b) the transmitted sound? Speed of sound in air is 340 m s–1 and in water 1486 m s–1.

        Answer

        (a) Frequency of the ultrasonic sound, ν = 1000 kHz = 106 Hz
        Speed of sound in air, va = 340 m/s
        The wavelength (λr) of the reflected sound is given by the relation:
        λr = v/v
        = 340/106 = 3.4 × 10-4 m.

        (b) Frequency of the ultrasonic sound, ν = 1000 kHz = 106 Hz
        Speed of sound in water, vw = 1486 m/s
        The wavelength of the transmitted sound is given as:
        λr = 1486 × 106 = 1.49 × 10-3 m.

        15.7. A hospital uses an ultrasonic scanner to locate tumours in a tissue. What is the wavelength of sound in the tissue in which the speed of sound is 1.7 km s–1? The operating frequency of the scanner is 4.2 MHz.

        Answer

        Speed of sound in the tissue, v = 1.7 km/s = 1.7 × 103 m/s
        Operating frequency of the scanner, ν = 4.2 MHz = 4.2 × 106 Hz
        The wavelength of sound in the tissue is given as:
        λ = v/v
        = 1.7 × 103 / 4.2 × 106 = 4.1 × 10-4 m.

        15.8. A transverse harmonic wave on a string is described by

        Where x and y are in cm and t in s. The positive direction of x is from left to right.

        (a) Is this a travelling wave or a stationary wave?
        If it is travelling, what are the speed and direction of its propagation?
        (b) What are its amplitude and frequency?
        (c) What is the initial phase at the origin?
        (d) What is the least distance between two successive crests in the wave?

        Answer

        (a) The equation of progressive wave travelling from right to left is given by the displacement function:
        y (x, t) = a sin (ωt + kx + Φ)     ….(i)
        The given equation is:

        On compaaring both the equations, we find that equation (ii) represents a travelling wave, propgating from right to left.
        Now using equations (i) and (ii), we can write:
        ω = 36 rad/s and k = 0.018 m-1
        We know that:
        v = ω/2π and λ = 2π/k

        Also,
        v = vλ
        ∴ v = (ω/2π) / (2π/k) = ω/k
        = 36/0.018 = 2000 cm/s = 20 m/s
        Hence, the speed of the given travelling wave is 20 m/s.

        (b) Amplitude of the given wave, a = 3 cm
        Frequency of the given wave:
        v = ω/2π = 36 / 2 × 3.14 = 573 Hz

        (c) On comparing equations (i) and (ii), we find that the intial phase angle, Φ = π/4

        (d) The distance between two successive crests or troughs is equal to the wavelength of the wave.
        Wavelength is given by the relation:
        k = 2π/λ

        ∴ λ = 2π/k = 2 × 3.14 / 0.018 = 348.89 cm =3.49 m.

        15.9. For the wave described in Exercise 15.8, plot the displacement (y) versus (t) graphs for x = 0, 2 and 4 cm. What are the shapes of these graphs? In which aspects does the oscillatory motion in travelling wave differ from one point to another: amplitude, frequency or phase?

        Answer

        All the waves have different phases.
        The given transverse harmonic wave is:

        For x = 0, the equation reduces to:
        Also,
        ω = 2π/t = 36rad/s-1

        ∴  t = π/18 s

        Now, plotting y vs. t graphs using the different values of t, as listed in the given table

        t (s)
        0
        T/8
        2T/7
        3T/8
        4T/8
        5T/8
        6T/8
        7T/8
        y (cm)
        3/√2
        3
        3/√2
        0
        -3/√2
        –3
        -3/√2
        0

        For x = 0, x = 2, and x = 4, the phases of the three waves will get changed. This is because amplitude and frequency are invariant for any change in x. The y–t plots of the three waves are shown in the given figure.

        15.10. For the travelling harmonic wave
        y (x, t) = 2.0 cos 2π (10t – 0.0080x + 0.35)

        Where x and y are in cm and t in s. Calculate the phase difference between oscillatory motion of two points separated by a distance of
        (a) 4 m,
        (b) 0.5 m,
        (c) λ/2
        (d) 3λ/4

        Answer

        Equation for a travelling harmonic wave is given as:
        y (x, t) = 2.0 cos 2π (10t – 0.0080x + 0.35)
        = 2.0 cos (20πt – 0.016πx + 0.70 π)
        Where,
        Propagation constant, k = 0.0160 π
        Amplitude, a = 2 cm
        Angular frequency, ω= 20 π rad/s
        Phase difference is given by the relation:
        Φ = kx = 2π/λ

        (a) For x = 4 m = 400 cm
        Φ = 0.016 π × 400 = 6.4 π rad

        (b) For 0.5 m = 50 cm
        Φ = 0.016 π × 50 = 0.8 π rad

        (c) For x = λ/2
        Φ = 2π/λ × λ/2 = π rad

        (d) For x = 3λ/4
        Φ = 2π/λ × 3λ/4 = 1.5π rad.

        Page No: 389

        15.11. The transverse displacement of a string (clamped at its both ends) is given by

        Where x and y are in m and t in s. The length of the string is 1.5 m and its mass is 3.0 ×10–2 kg.
        Answer the following:
        (a) Does the function represent a travelling wave or a stationary wave?
        (b) Interpret the wave as a superposition of two waves travelling in opposite directions. What is the wavelength, frequency, and speed of each wave?
        (c) Determine the tension in the string.

        Answer

        (a) The general equation representing a stationary wave is given by the displacement function:
        y (x, t) = 2a sin kx cos ωt
        This equation is similar to the given equation:

        Hence, the given equation represents a stationary wave.
        (b) A wave travelling along the positive x-direction is given as:
        y1 = a sin (ωt – kx)
        The wave travelling along the positive x-direction is given as:
        y2 = a sin (ωt + kx)
        The supposition of these two waves yields:
        y = y1 + y2 = a sin (ωt – kx) – a sin (ωt + kx)
        = a sin (ωt) cos (kx) – a sin (kx) cos (ωt) –  a sin (ωt) cos (kx) – a sin (kx) cos (ωt)
        = 2 a sin (kx) cos (ωt)

        ∴Wavelength, λ = 3 m
        It is given that:
        120π = 2πν
        Frequency, ν = 60 Hz
        Wave speed, v = νλ
        = 60 × 3 = 180 m/s

        (c) The velocity of a transverse wave travelling in a string is given by the relation:
        v = √T/µ              ….(i)
        where,
        Velocity of the transverse wave, v = 180 m/s
        Mass of the string, m = 3.0 × 10–2 kg
        Length of the string, l = 1.5 m
        Mass per unit length of the string, µ = m/l
        = 3.0 × 1.5 = 10-2
        = 2 × 10-2 kg m-1

        Tension in the string = T
        From equation (i), tension can be obtained as:
        T = v2μ
        = (180)2 × 2 × 10–2
        = 648 N 

        15.12. (i) For the wave on a string described in Exercise 15.11, do all the points on the string oscillate with the same (a) frequency, (b) phase, (c) amplitude? Explain your answers. (ii) What is the amplitude of a point 0.375 m away from one end?

        Answer

        All the points on the string
        (i) have the same frequency except at the nodes (where frequency is zero)
        (ii) have thse same phase everywhere in one loop except at the nodes.
        However, the amplitude of vibration at different points is different.

        15.13. Given below are some functions of x and t to represent the displacement (transverse or longitudinal) of an elastic wave. State which of these represent (i) a traveling wave, (ii) a stationary wave or (iii) none at all:

        (a) y = 2 cos (3x) sin (10t)
        (b) y = 2 √x – vt
        (c)  y = 3 sin (5x – 0.5t) + 4 cos (5x – 0.5t) (d) y = cos x sin t + cos 2x sin 2t

        Answer

        (a) The given equation represents a stationary wave because the harmonic terms kx and ωt appear separately in the equation.
        (b) The given equation does not contain any harmonic term. Therefore, it does not represent either a travelling wave or a stationary wave.
        (c) The given equation represents a travelling wave as the harmonic terms kx and ωt are in the combination of kx – ωt.
        (d) The given equation represents a stationary wave because the harmonic terms kx and ωt appear separately in the equation. This equation actually represents the superposition of two stationary waves.

        15.14. A wire stretched between two rigid supports vibrates in its fundamental mode with a frequency of 45 Hz. The mass of the wire is 3.5 × 10–2 kg and its linear mass density is 4.0 × 10–2 kg m–1. What is (a) the speed of a transverse wave on the string, and (b) the tension in the string?

        Answer

        (a) Mass of the wire, m = 3.5 × 10–2 kg
        Linear mass density, μ = m/l = 4.0 × 10-2 kg m-1
        Frequency of vibration, v = 45 Hz∴ length of the wire, l = m/μ = 3.5 × 10–2 / 4.0 × 10-2 = 0.875 m
        The wavelength of the stationary wave (λ) is related to the length of the wire by the relation:
        λ = 2l/m
        where,
        n = Number of nodes in the wire
        For fundamental node, n = 1:
        λ = 2l
        λ = 2 × 0.875 = 1.75 m
        The speed of the transverse wave in the string is given as:
        v = νλ= 45 × 1.75 = 78.75 m/s

        (b) The tension produced in the string is given by the relation:
        T = v2µ
        = (78.75)2 × 4.0 × 10–2 = 248.06 N

        15.15. A metre-long tube open at one end, with a movable piston at the other end, shows resonance with a fixed frequency source (a tuning fork of frequency 340 Hz) when the tube length is 25.5 cm or 79.3 cm. Estimate the speed of sound in air at the temperature of the experiment. The edge effects may be neglected.

        Answer

        Frequency of the turning fork, ν = 340 Hz
        Since the given pipe is attached with a piston at one end, it will behave as a pipe with one end closed and the other end open, as shown in the given figure.

        Such a system produces odd harmonics. The fundamental note in a closed pipe is given by the relation:

        l1 = π/4
        where,

        length of pipe, l1 = 25.5 cm = 0.255 m
        ∴ λ = 4l1 = 4 × 0.255 = 1.02 m
        The speed of the sound is given by the relation:
        v = vλ = 340 × 1.02 = 346.8 m/s.

        15.16. A steel rod 100 cm long is clamped at its middle. The fundamental frequency of longitudinal vibrations of the rod is given to be 2.53 kHz. What is the speed of sound in steel?

        Answer

        Length of the steel rod, l = 100 cm = 1 m
        Fundamental frequency of vibration, ν = 2.53 kHz = 2.53 × 103 Hz
        When the rod is plucked at its middle, an antinode (A) is formed at its centre, and nodes (N) are formed at its two ends, as shown in the given figure.

        The distance between two successive node is λ/2
        ∴ l = λ/2
        λ = 2l = 2 × l = 2 m

        The speed of sound in steel is given by the relation:
        v = νλ
        = 2.53 × 103 × 2
        = 5.06 × 103 m/s
        = 5.06 km/s

        15.17. A pipe 20 cm long is closed at one end. Which harmonic mode of the pipe is resonantly excited by a 430 Hz source? Will the same source be in resonance with the pipe if both ends are open? (Speed of sound in air is 340 m s–1).

        Answer

        First (Fundamental); No
        Length of the pipe, l = 20 cm = 0.2 m
        Source frequency = nth normal mode of frequency, νn = 430 Hz
        Speed of sound, v = 340 m/s
        In a closed pipe, the nth normal mode of frequency is given by the relation:

        Hence, the first mode of vibration frequency is resonantly excited by the given source.

        In a pipe open at both ends, the nth mode of vibration frequency is given by the relation:
        vn = nv/2l
        n = 2lvn/v

        15.18. Two sitar strings A and B playing the note ‘Ga’ are slightly out of tune and produce beats of frequency 6 Hz. The tension in the string A is slightly reduced and the beat frequency is found to reduce to 3 Hz. If the original frequency of A is 324 Hz, what is the frequency of B?

        Answer

        Frequency of string A, fA = 324 Hz
        Frequency of string B = fB
        Beat’s frequency, n = 6 Hz
        Beat’s Frequency is given as:

        Frequency decreases with a decrease in the tension in a string. This is because frequency is directly proportional to the square root of tension. It is given as:
        v ∝ √T
        Hence, the beat frequency cannot be 330 Hz

        ∴ fB = 318 Hz. 

        15.19. Explain why (or how):
        (a) In a sound wave, a displacement node is a pressure antinode and vice versa,
        (b) Bats can ascertain distances, directions, nature, and sizes of the obstacles without any “eyes”,
        (c) A violin note and sitar note may have the same frequency, yet we can distinguish between the two notes,
        (d) Solids can support both longitudinal and transverse waves, but only longitudinal waves can propagate in gases, and
        (e) The shape of a pulse gets distorted during propagation in a dispersive medium.

        Answer

        (a) A node (N) is a point where the amplitude of vibration is the minimum and pressure is the maximum.
        An antinode (A) is a point where the amplitude of vibration is the maximum and pressure is the minimum.
        Therefore, a displacement node is nothing but a pressure antinode, and vice versa.

        (b) Bats emit ultrasonic waves of large frequencies. When these waves are reflected from the obstacles in their path, they give them the idea about the distance, direction, size and nature of the obstacle.

        (c) The overtones produced by a sitar and a violin, and the strengths of these overtones, are different. Hence, one can distinguish between the notes produced by a sitar and a violin even if they have the same frequency of vibration.

        (d) This is because solids have both, the elasticity of volume and elasticity of shape, whereas gases have only the volume elasticity.

        (e) A sound pulse is a combination of waves of different wavelength. As waves of different λ travel in a dispersive medium with different velocities, therefore, the shape of the pulse gets distorted.

        15.20. A train, standing at the outer signal of a railway station blows a whistle of frequency 400 Hz in still air. (i) What is the frequency of the whistle for a platform observer when the train (a) approaches the platform with a speed of 10 m s–1, (b) recedes from the platform with a speed of 10 m s–1? (ii) What is the speed of sound in each case? The speed of sound in still air can be taken as 340 m s–1.

        Answer

        (i) (a)Frequency of the whistle, ν = 400 Hz
        Speed of the train, vT= 10 m/s
        Speed of sound, v = 340 m/s
        The apparent frequency (v’) of the whistle as the train approaches the platform is given by the
        relation:

        (ii) The apparent change in the frequency of sound is caused by the relative motions of the source and the observer. These relative motions produce no effect on the speed of sound. Therefore, the speed of sound in air in both the cases remains the same, i.e., 340 m/s.

        15.21. A train, standing in a station-yard, blows a whistle of frequency 400 Hz in still air. The wind starts blowing in the direction from the yard to the station with at a speed of 10 m s–1. What are the frequency, wavelength, and speed of sound for an observer standing on the station’s platform? Is the situation exactly identical to the case when the air is still and the observer runs towards the yard at a speed of 10 m s–1? The speed of sound in still air can be taken as 340 m s–1.

        Answer

        For the stationary observer:
        Frequency of the sound produced by the whistle, ν = 400 Hz
        Speed of sound = 340 m/s
        Velocity of the wind, v = 10 m/s
        As there is no relative motion between the source and the observer, the frequency of the sound heard by the observer will be the same as that produced by the source, i.e., 400 Hz.
        The wind is blowing toward the observer. Hence, the effective speed of the sound increases by 10 units, i.e.,
        Effective speed of the sound, ve = 340 + 10 = 350 m/s
        The wavelength (λ) of the sound heard by the observer is given by the relation:
        λ = ve/v = 350/400 = 0.875 m
        For the running observer:
        Velocity of the observer, vo = 10 m/s
        The observer is moving toward the source. As a result of the relative motions of the source and the observer, there is a change in frequency (v‘).
        This is given by the relation:

        Since the air is still, the effective speed of sound = 340 + 0 = 340 m/s
        The source is at rest. Hence, the wavelength of the sound will not change, i.e., λ remains 0.875 m.
        Hence, the given two situations are not exactly identical.

        Additional Excercises

        15.22. A travelling harmonic wave on a string is described by

        (a) What are the displacement and velocity of oscillation of a point at x = 1 cm, and t = 1 s? Is this velocity equal to the velocity of wave propagation?
        (b) Locate the points of the string which have the same transverse displacements and velocity as the x = 1 cm point at t = 2 s, 5 s and 11 s.

        Answer

        (a) The given harmonic wave is

        = 90 coss (732.81°) = 90 cos (90 × 8 + 12.81°)
        = 90 cos (12.81°)
        = 90 × 0.975 =87.75 cm/s
        Now, the equation of a propagating wave is given by:
        y (x, t) = asin (kx + wt + Φ)

        where,
        k = 2π/λ
        ∴ λ = 2π/k
        and, ω = 2πv
        ∴ v = ω/2π
        Speed, v = vλ = ω/k
        where,
        ω = 12rad/s
        k = 0.0050 m-1
        ∴ v = 12/0.0050 = 2400 cm/s
        Hence, the velocity of the wave oscillation at x = 1 cm and t = 1s is not equal to the velocity of the wave propagation.

        (b) Propagation constant is related to wavelength as:
        k = 2π/λ
        ∴ λ = 2π/k = 2 × 3.14 / 0.0050
        = 1256 cm = 12.56 m
        Therefore, all the points at distance nλ (n = ±1, ±2, …. and so on), i.e. ± 12.56 m, ± 25.12 m, … and so on for x = 1 cm, will have the same displacement as the x = 1 cm points at t = 2 s, 5 s, and 11 s.

        15.23. A narrow sound pulse (for example, a short pip by a whistle) is sent across a medium. (a) Does the pulse have a definite (i) frequency, (ii) wavelength, (iii) speed of propagation? (b) If the pulse rate is 1 after every 20 s, (that is the whistle is blown for a split of second after every 20 s), is the frequency of the note produced by the whistle equal to 1/20 or 0.05 Hz?

        Answer

        (a) A short pip be a whistle has neither a definite wavelength nor a definite frequency. However, its speed of propagation is fized, being equal to speed of sound in air.

        (b) No, frequency of the note produced by a whistle is not 1/20 = 0.05 Hz. Rather 0.05 Hz is the frequency of repetition of the short pip of the whistle.

        15.24. One end of a long string of linear mass density 8.0 × 10–3 kg m–1 is connected to an electrically driven tuning fork of frequency 256 Hz. The other end passes over a pulley and is tied to a pan containing a mass of 90 kg. The pulley end absorbs all the incoming energy so that reflected waves at this end have negligible amplitude. At t = 0, the left end (fork end) of the string x = 0 has zero transverse displacement (y = 0) and is moving along positive y-direction. The amplitude of the wave is 5.0 cm. Write down the transverse displacement y as function of x and t that describes the wave on the string.

        Answer

        The equation of a travelling wave propagating along the positive y-direction is given by the displacement equation:
        y (x, t) = a sin (wt – kx) … (i)
        Linear mass density, μ = 8.0 × 10-3 kg m-1

        Frequency of the tuning fork, ν = 256 Hz
        Amplitude of the wave, a = 5.0 cm = 0.05 m … (ii)
        Mass of the pan, m = 90 kg
        Tension in the string, T = mg = 90 × 9.8 = 882 N
        The velocity of the transverse wave v, is given by the relation:

        Substituting the values from equations (ii), (iii), and (iv) in equation (i), we get the displacement equation:
        y (x, t) = 0.05 sin (1.6 × 103t – 4.84 x) m.

        15.25. A SONAR system fixed in a submarine operates at a frequency 40.0 kHz. An enemy submarine moves towards the SONAR with a speed of 360 km h–1. What is the frequency of sound reflected by the submarine? Take the speed of sound in water to be 1450 m s–1.

        Answer

        Operating frequency of the SONAR system, ν = 40 kHz
        Speed of the enemy submarine, ve = 360 km/h = 100 m/s
        Speed of sound in water, v = 1450 m/s
        The source is at rest and the observer (enemy submarine) is moving toward it. Hence, the apparent frequency (v‘) received and reflected by the submarine is given by the relation:

        15.26. Earthquakes generate sound waves inside the earth. Unlike a gas, the earth can experience both transverse (S) and longitudinal (P) sound waves. Typically the speed of S wave is about 4.0 km s–1, and that of P wave is 8.0 km s–1. A seismograph records P and S waves from an earthquake. The first P wave arrives 4 min before the first S wave. Assuming the waves travel in straight line, at what distance does the earthquake occur?

        Answer

        Let vSand vP be the velocities of S and P waves respectively.
        Let L be the distance between the epicentre and the seismograph.
        We have:
        L = vStS          …(i)
        L = vPtP         …(ii)
        Where,
        tS and tP are the respective times taken by the S and P waves to reach the seismograph from the epicentre
        It is given that:
        vP = 8 km/s
        vS = 4 km/s
        From equations (i) and (ii), we have:
        vS tS = vP tP
        4tS = 8 tP
        tS = 2 tP         …(iii)
        It is also given that:
        tS – tP = 4 min = 240 s
        2tP – tP = 240
        tP = 240
        And tS = 2 × 240 = 480 s
        From equation (ii), we get:
        L = 8 × 240
        = 1920 km
        Hence, the earthquake occurs at a distance of 1920 km from the seismograph.

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