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Wave Optics

 1. The locus of all particles of the medium vibrating in the same phase at a  given instant is known as wavefront . Depending on the shape ...

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Thursday, 13 January 2022

Wave Optics

  January 13, 2022 Lakshman Jangid   Physics 12   No comments

 1. The locus of all particles of the medium vibrating in the same phase at a  given instant is known as wavefront. Depending on the shape of sources of light, wavefront can be of three types.

2. Spherical wavefront: When the source of light is a point source, the wavefront is spherical.

3. Cylindrical wavefront: When the source of light is linear, the wavefront is cylindrical.

4. Plane wavefront: When the point source or linear source of light is at a very large distance, a small portion of the spherical or cylindrical wavefront appears to be plane. Such a wavefront is known as a plane wavefront.

5. Huygens principle: According to Huygens principle, (a) Every point on a given wavefront (primary wavefront) acts as a fresh source of new disturbance, called secondary wavelets. (b) The secondary wavelets spread out in all directions with the speed of light in the medium. A surface touching these secondary wavelets tangentially in the forward direction at any instant gives the new (secondary) wavefront at that instant.

6. Huygen's principle can be used to verify laws of reflection and refraction.

7. The sources of light, which emit continuously light waves of the same wavelength (monochromatic light), same frequency, and in the same phase or have a constant phase difference with time are known as coherent sources. Two sources of light that do not emit light waves with a constant phase difference are called incoherent sources. 


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Saturday, 1 January 2022

Dual Nature of Matter and Radiation

  January 01, 2022 Lakshman Jangid   Physics 12   No comments

 1.  Quantum mechanics is a mathematical model that describes the behavior of the particles on an atomic and subatomic scale.

2. According to Planck's quantum theory, the Energy of light comes in form of packets (it is not a material particle). These packets are called Quanta or Photons.

3. Energy of the photon depends on frequency. Frequency does not change with changing medium. Energy is given by \[ E = hf = (6.636 \times 10^{-34})f\] 

4. Energy of the photon having wavelength $ \lambda $ is given by \[ E = \frac{hc}{\lambda} = \frac{12400}{\lambda (\ in \ Angstrom)}eV  \] and momentum of photon is given by \[  p = \frac{h}{\lambda}  \] where $ h $ is plack's constant and $ c $ is speed of light.

5. Photons are electrically neutral particles. These are not deflected by the electric and magnetic fields.

6. Photons can collide with material particles like electrons. During the collision, total Energy and total momentum remain constant i.e. collision is elastic.   

7. Rest mass of the photon is zero. This means that photon does not exist at rest. Equivalent mass of the photon is given by, \[ m = \frac{hf}{c^2} \]

8. Intensity is defined as energy radiated per unit time per unit area. i.e. \[ I = \frac{E}{tA}= \frac{P}{A} \] where P is power. SI unit of intensity is  $  \frac{W}{m^2} $.

9. A source is at power P and emitting radiation energy of wavelength $ \lambda $ then number of photons emitted by the source per second is given by, \[ n = \frac{P}{E}= \frac{P \lambda}{hc} \] 

10. Photon Flux is the number of photons incident on a surface normally per second per unit area. \[ Photon \ Flux, \phi = \frac{Intensity}{Energy \ of \ a \ photon} = \frac{I\lambda}{hc} \]

11. When radiation is incident on the surface then it will apply some force on the surface.  If radiation falls on the surface at some angle and is reflected by the surface, the average force is given by, \[  F = \frac{2IAcos^2\theta}{c} \]Radiation pressure is given by, \[ P = \frac{2Icos^2\theta}{c} \]


Study of Photoelectric Effect

12. Minimum energy required to escape an electron from the surface is known as Work Function $ \phi $.  The minimum frequency of incident light that is just capable of ejecting electrons from metal is called the threshold frequency.
        Metal            Work Function (eV)
        Cesium                    1.9
        Potassium                2.2
        Sodium                    2.3
        Lithium                    2.5
        Calcium                   3.2
        Copper                     4.5
        Silver                       4.7
        Platinum                  5.6

13. When electromagnetic radiation of suitable wavelength is incident on the metal surface such that electrons emitted from the surface, this phenomenon is known as Photoelectric emission.

14. When energy is given in form of heat to the metal surface such that electrons are emitted from the surface, this phenomenon is known as Thermionic emission.

15. When the strong field is applied in such a way that electrons get accelerated and overcome the potential barrier, this phenomenon is known as Field emission.

16. The phenomenon of the photoelectric effect was discovered by Heinrich Hertz in 1887. While performing an experiment for the production of electromagnetic waves by means of spark discharge. Hertz observed that sparks occurred more rapidly in the air gap of his transmitter when ultraviolet radiations were directed at one of the metal plates. Hertz could not explain his observations.

17. Phillip Lenard observed that when ultraviolet radiations were made incident on the emitter plate of an evacuated glass tube enclosing two metal plates (called electrodes), current flows in the circuit, but as soon as ultraviolet radiation falling on the emitter plate was stopped, the current flow stopped. These observations indicate that when ultraviolet radiations fall on the emitter (cathode) plate, the electrons are ejected from it, which are attracted towards the anode plate. The electrons flow through the evacuated glass tube, complete the circuit and current begins to flow in the circuit.

18. Hallwachs studied further by taking a plate and an electroscope. The zinc plate was connected to an electroscope. He observed that: (i) When an uncharged zinc plate was irradiated by ultraviolet light, the zinc plate acquired a positive charge. (ii) When a positively charged zinc plate is illuminated by ultraviolet light, the positive charge of the plate was increased. (iii) When a negatively charged zinc plate was irradiated by ultraviolet light, the zinc plate lost its charge. All these observations show that when ultraviolet light falls on zinc plate, the negatively charged particles (electrons) are emitted.

19. Einstein's Photoelectric equation is \[ hf = \phi + KE \implies \frac{1}{2}mv^2 = hf - \phi \]where f is incident frequency and v is maximum velocity of the electron.

20. Photoelectric current is directly proportional to the intensity of the incident light keeping frequency and potential the same. On increasing the intensity, photoelectric current will increase and vice-versa. It does not depend on the incident energy.

21.  If the collector is given negative potential with respect to the emitter, then at some potential electrons will not reach the collector. Due to this, there will be no current in the circuit. If the potential of the collector is further increased in the negative, no current will be in the circuit. This potential at which the photoelectric current is zero is known as Stopping Potential. \[ eV_0 = K.E. = \frac{1}{2}mv^2 \]Stopping potential is independent of the intensity of the incident light. It depends only on the incident energy. 

22. Kinetic energy of the electrons depends only on the incident energy, not on the intensity of the incident light.

23. There is no time lag between the incidence of light and the emission of photoelectrons.

24. De Broglie gave the wavelength associated with moving object, which is given by, \[ \lambda = \frac{h}{mv} = \frac{h}{p}  \]where m is mass of the object and v is the speed of the object. 

25. If E is the kinetic energy of the electron, then the De-Broglie wavelength of the electron will be \[ \lambda = \frac{h}{\sqrt{2mE}} \] 

26. If electron is accelerated by potential V then De-Broglie wavelength of electron will be \[ \lambda = \frac{h}{\sqrt{2meV}} \]

27. Davisson and Germer Experiment gives the experimental evidence for the wave nature of the electrons.

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Friday, 7 May 2021

Physics Syllabus class 11

  May 07, 2021 Lakshman Jangid   No comments

CBSE SYLLABUS (2018-19)

Unit I: Physical World and Measurement

Chapter–1: Physical World Physics-scope and excitement; nature of physical laws; Physics, technology and society. 

Chapter–2: Units and Measurements Need for measurement: Units of measurement; systems of units; SI units, fundamental and derived units. Length, mass and time measurements; accuracy and precision of measuring instruments; errors in measurement; significant figures. Dimensions of physical quantities, dimensional analysis and its applications. 

Unit II: Kinematics 

Chapter–3: Motion in a Straight Line Frame of reference, Motion in a straight line: Position-time graph, speed and velocity. Elementary concepts of differentiation and integration for describing motion, uniform and non-uniform motion, average speed and instantaneous velocity, uniformly accelerated motion, velocity - time and position-time graphs. Relations for uniformly accelerated motion (graphical treatment). 

Chapter–4: Motion in a Plane Scalar and vector quantities; position and displacement vectors, general vectors and their notations; equality of vectors, multiplication of vectors by a real number; addition and subtraction of vectors, relative velocity, Unit vector; resolution of a vector in a plane, rectangular components, Scalar and Vector product of vectors. Motion in a plane, cases of uniform velocity and uniform acceleration-projectile motion, uniform circular motion. 

Unit III: Laws of Motion 

Chapter–5: Laws of Motion Intuitive concept of force, Inertia, Newton's first law of motion; momentum and Newton's second law of motion; impulse; Newton's third law of motion. Law of conservation of linear momentum and its applications. Equilibrium of concurrent forces, Static and kinetic friction, laws of friction, rolling friction, lubrication. Dynamics of uniform circular motion: Centripetal force, examples of circular motion (vehicle on a level circular road, vehicle on a banked road). 

Unit IV: Work, Energy, and Power

Chapter–6: Work, Engery and Power Work done by a constant force and a variable force; kinetic energy, work-energy theorem, power. Notion of potential energy, potential energy of a spring, conservative forces: conservation of mechanical energy (kinetic and potential energies); non-conservative forces: motion in a vertical circle; elastic and inelastic collisions in one and two dimensions. 

Unit V: Motion of System of Particles and Rigid Body

Chapter–7: System of Particles and Rotational Motion Centre of mass of a two-particle system, momentum conservation and center of mass motion. Centre of mass of a rigid body; centre of mass of a uniform rod. Moment of a force, torque, angular momentum, law of conservation of angular momentum and its applications. Equilibrium of rigid bodies, rigid body rotation and equations of rotational motion, comparison of linear and rotational motions. Moment of inertia, radius of gyration, values of moments of inertia for simple geometrical objects (no derivation). Statement of parallel and perpendicular axes theorems and their applications. 

Unit VI: Gravitation  

Chapter–8: Gravitation Kepler's laws of planetary motion, universal law of gravitation. Acceleration due to gravity and its variation with altitude and depth. Gravitational potential energy and gravitational potential, escape velocity, orbital velocity of a satellite, Geo-stationary satellites. 

Unit VII: Properties of Bulk Matter 

Chapter–9: Mechanical Properties of Solids Elastic behaviour, Stress-strain relationship, Hooke's law, Young's modulus, bulk modulus, shear modulus of rigidity, Poisson's ratio; elastic energy. 

Chapter–10: Mechanical Properties of Fluids Pressure due to a fluid column; Pascal's law and its applications (hydraulic lift and hydraulic brakes), effect of gravity on fluid pressure. Viscosity, Stokes' law, terminal velocity, streamline and turbulent flow, critical velocity, Bernoulli's theorem and its applications. Surface energy and surface tension, angle of contact, excess of pressure across a curved surface, application of surface tension ideas to drops, bubbles and capillary rise. 

Chapter–11: Thermal Properties of Matter Heat, temperature, thermal expansion; thermal expansion of solids, liquids and gases, anomalous expansion of water; specific heat capacity; Cp, Cv - calorimetry; change of state - latent heat capacity. Heat transfer-conduction, convection and radiation, thermal conductivity, qualitative ideas of Blackbody radiation, Wein's displacement Law, Stefan's law, Greenhouse effect. 

Unit VIII: Thermodynamics

Chapter–12: Thermodynamics Thermal equilibrium and definition of temperature (zeroth law of thermodynamics), heat, work, and internal energy. First law of thermodynamics, isothermal and adiabatic processes. Second law of thermodynamics: reversible and irreversible processes, Heat engine and refrigerator. 

Unit IX: Behaviour of Perfect Gases and Kinetic Theory of Gases  

Chapter–13: Kinetic Theory Equation of state of a perfect gas, work done in compressing a gas. Kinetic theory of gases - assumptions, concept of pressure. Kinetic interpretation of temperature; rms speed of gas molecules; degrees of freedom, law of equi-partition of energy (statement only) and application to specific heat capacities of gases; concept of mean free path, Avogadro's number. 

Unit X: Mechanical Waves and Ray Optics  

Chapter–14: Oscillations and Waves Periodic motion - time period, frequency, displacement as a function of time, periodic functions. Simple harmonic motion (S.H.M) and its equation; phase; oscillations of a loaded springrestoring force and force constant; energy in S.H.M. Kinetic and potential energies; simple pendulum derivation of expression for its time period. Free, forced and damped oscillations (qualitative ideas only), resonance. Wave motion: Transverse and longitudinal waves, speed of wave motion, displacement relation for a progressive wave, principle of superposition of waves, reflection of waves, standing waves in strings and organ pipes, fundamental mode and harmonics, Beats, Doppler effect. 

Chapter–15: RAY OPTICS: Reflection of light, spherical mirrors, mirror formula, refraction of light, total internal reflection and its applications, optical fibres, refraction at spherical surfaces, lenses, thin lens formula, lensmaker's formula, magnification, power of a lens, combination of thin lenses in contact, refraction and dispersion of light through a prism. Scattering of light - blue colour of sky and reddish apprearance of the sun at sunrise and sunset. Optical instruments: Microscopes and astronomical telescopes (reflecting and refracting) and their magnifying powers.

**Syllabus taken from cbse website.

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Tuesday, 4 May 2021

Unit and Dimensions: Problems

  May 04, 2021 Lakshman Jangid   No comments
1. In SI system, the unit of Temperature is
    (a) Degree Celcius
    (b) Degree Centigrade
    (c) Degree Kelvin
    (d) Degree Fahrenheit 
[d]

2. Which of the following is a unit of distance?
     (a) Metre
     (b) Astronomical unit
     (c) Light year
     (d)  All of the above
[d]

3. What is the dimension of surface tension:
     (a) $[M^2L^2T^{-2} $
     (b) $[M^2LT^{-2}]$
     (c) $ [ML^0T^{-2}]$
     (d) None of these
[c]

4. Which of the following have the same dimensions?
     (a) Stress
     (b) Bulk modulus
     (c) Thrust
     (d) Energy Density
[a and b]

5. If C and R denote the capacitance and resistance, then the dimension of RC is:
     (a) $[M^0L^0T ]$
     (b) $[ML^0T] $
     (c)  $[MLT]$
     (d)  $[M^0L^0T^2]$
[a]

6. Write any two physical quantities which have the dimension of Energy? [Torque, Work]

7. Is it possible to add any two physical quantities? [No]

8. Force on a sphere of radius 'a' moving in the medium with velocity 'v' is given by $F = 6\pi \eta av $. Find the dimension of $ \eta $. [$ML^{-1}T^{-1}$]

9. What is the dimensional formula for Planck's constant? [$ML^2T^{-1}$]

10. In the formula, $X = 3YZ^2$, X and Z have the dimensions of capacitance and magnetic induction respectively. Find the dimension of Y in MKSQ system. [$M^{-3}L^{-2}T^{4}Q^{4}$]

11. The equation of state for a real gas is given by $ (p+\frac{a}{V^2})(v-b) = RT $. Find the dimensions of 'a' and 'b'. [$[ML^5T^{-2}]$, $[L^3]$]

12. Find the dimension of $\frac{1}{2}\epsilon_0 E^2$. [$ML^{-1}T^{-2}$]

13. A quantity X is given by $ \epsilon_0 L\frac{\Delta V}{\Delta t} $ where $\epsilon_0 $ is the permittivity of the free space, L is the length,  $\Delta$V is the potential difference and ${\Delta t}$ is a time interval. The dimensional formula for X is the same as that of  (a) Resistance (b) Charge (c) Voltage (d) Current. [d]

14. Pressure depends on distance as $ p = \frac{\alpha}{\beta}e^{-\frac{\alpha z}{k \theta}} $, where $\alpha$, $\beta$ are constant, z is the distance, k is Boltzman's constant and $\theta$ is temperature. Find the dimension of $\beta$. [$L^{2}$]

15. Which of the following pair (s) has the same dimension?
     (a) Torque and work
     (b) Angular momentum and Work
     (c) Energy and Young's modulus
     (d) Light-year and Wavelength 
     (e) Reynold number and co-efficient of friction
     (f) Curie and Frequency of the light wave
     (g) Latent heat and gravitational potential
     (h) Planck's constant and torque
[a,d,e,f,g]

16. Let $ [\epsilon_0]$ denote the dimensional formula of permittivity of the vacuum, and $[\mu_0]$ that of permeability of the vacuum. Find their dimensional formula in term of mass M, length L, time T, and electric current I. [$\epsilon_0 = [M^{-1}L^{-3}T^4I^2]$, $\mu_0= [MLT^{-2}I^{-2}]$]

17. Planck's constant h, speed of light c, and gravitational constant G are used to form a unit of length L and a unit of mass M. Then find the correct option (s) is (are): 
   (a) $M \propto \sqrt{c}$ 
   (b) $M \propto \sqrt{G}$ 
   (c) $L \propto \sqrt{h}$ 
   (d) $L \propto \sqrt{G}$
[a,c,d]

18. In term of potential difference V, electric current I, permittivity $\epsilon_0$, permeability $\mu_0$ and speed of light c, the dimensionally correct equation(s) is(are):
    (a) $\mu_0 I^2 = \epsilon_0V^2$ 
    (b) $ \mu_0 I = \epsilon_0V$ 
    (c) $ I = \epsilon_0 cV$ 
    (d) $ \mu_0 c I = \epsilon_0 V$ 
[a,c]

19. A length-scale (l) depends on the permittivity ($\epsilon $) of a dielectric material. Boltzmann constant ($k_B$), the absolute temperature (T), the number per unit volume (n) of certain charged particles, and charge (q) carried by each of the particles. Which of the following expression(s) for l is/are dimensionally correct? 
    (a) $l = \sqrt{\frac{nq^2}{\epsilon k_B T}}$ 
    (b) $l = \sqrt{\frac{\epsilon k_B T}{nq^2}} $ 
    (c) $ l = \sqrt{\frac{q^2}{\epsilon n^{2/3}k_B T}}$ 
    (d) $l = \sqrt{\frac{q^2}{\epsilon n^{1/3}k_B T}}$
[b,d]

20. Give the MKS unit of each of the following: 
    (a) Young's Modulus
    (b) Magnetic Induction
    (c) Power of lens
[$N/m^2$, Tesla, Dioptre]

21. A gas bubble, from an explosion underwater, oscillate with a period T proportional to $p^ad^bE^c$, where  'P' is the static pressure, 'd' is the density of the water, and 'E' is the total energy of the explosion. Find the values of a, b, and c. [$a = -\frac{5}{6},b=\frac{1}{2},c=\frac{1}{3}$]

22. Write the dimensions of the following in terms of mass, time, length, and charge
    (a) Magnetic flux 
    (b) Rigidity modulus
[$[ML^2T^{-1}Q^{-1}], [ML^{-1}T^{-2}]$]

23. Match the following with their dimensions where Q is for charge:

Column I

Column II

(A) Angular momentum

(a) $[ML^2T^{-2}]$

(B) Latent Heat

(b) $[ML^2Q^{-2}]$

(C) Torque

(c) $[ML^2T^{-1}]$

(D) Capacitance

(d) $[ML^3T^{-1}Q^{-2}]$

(E) Inductance

(e) $[M^{-1}L^{-2}T^{2}Q^2]$

(F) Resistivity

(f) $[L^2T^{-2}]$

[$(A) \to (c),(B) \to (f) ,(C)\to (a), (D)\to (e), (E)\to (b),(F)\to (d)$]

24. Match column I with column II:

Column I

Column II

(A) Capacitance

(i)                  Ohm-second

(B) Inductance

(ii)                Coulomb2-joule-1

(C) Magnetic Induction

(iii)               Coulomb (volt)-1

 

(iv)               Newton (amp-metre)-1

 

(v)                Volt-second (ampere)-1

[$(A) \to (ii),(iii), (B)\to (i),(v), (C)\to (iv)$]
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Monday, 26 April 2021

Mathematics for Physics II

  April 26, 2021 Lakshman Jangid   No comments

Geometry

1. Two triangles are similar when the ratio of sides is same and angles are same. If two triangles have same configuration i.e. same sides and same angles, then triangles are congruent.

2. Vertical opposite angles are equal.

3. Alternate angles are equal.

4. General Equation of the line is $ y = mx + c$ where m is the slope and c is the intercept.

5. Slope of any line passing through points $ (x_1, y_1) $ and $ (x_2, y_2) $ is $ m = \frac{y_2-y_1}{x_2-x_1} $. Slope is inclination of the line with positive x-axis. If $ \theta $ is the angle made by the line with positive x-axis then slope will be $ m = tan\theta $. For horizontal line, slope is 0 and for vertical line, slope is $ \infty $. 

6. Equation of line passing through points $ (x_1, y_1) $ and $ (x_2, y_2) $ is $ (y-y_1) = \frac{y_2-y_1}{x_2-x_1} (x-x_1) $

7. If we are given two lines, then lines $y=m_1x+c_1$ and $y=m_2x+c_2$ are parallel only when these have the same slopes, i.e. $m_1 = m_2 $. 

8. Two lines $y=m_1x+c_1$ and $y=m_2x+c_2$ are perpendicular when the product of the slopes of two lines is -1, i.e. $m_1m_2 = -1$.

9. Equation of the circle is of form, $ ax^2 + ay^2 + 2bx + 2cy + d = 0 $.

10. Equation of the parabola is either of the form $ (y-c)^2=4a(x-b) $, or $ (x-c)^2 = 4a(y-b) $ or $ y = ax^2 - bx $ or $ x = ay^2-by $.

11. Equation of ellipse is $ \frac{x^2}{a^2}+ \frac{y^2}{b^2}  = 1 $.

12. Equation of hyperbola is $\frac{x^2}{a^2} - \frac{y^2}{b^2}  = 1 $. 


Calculus

1. Function is defined as a operation in which element of the set first are related to elements of second set by some relation. 

Domain of the function is the set all elements (values) which function can take. Range is set of values which function can give. 

Let any function $ y = f(x) $. Let us consider that curve $ y=f(x) $ passes through $(x,y) $. If we need to find the tangent at this point, then slope of the curve will be given by $ m = \frac{dy}{dx}=\frac{d f(x)}{dx} = f'(x) $ where $ \frac{dy}{dx}$ is derivative of y with respect to x.

Derivative of some functions are given below:

1. $ y = constant \implies \frac{dy}{dx}=0$

2. $ y = x^n  \implies \frac{dy}{dx} = nx^{n-1} $ 

3. $ y = sinx \implies \frac{dy}{dx}=cosx$

4. $ y = cosx \implies \frac{dy}{dx}= -sinx $

5. $ y = tanx \implies \frac{dy}{dx}= sec^2x $

6. $ y = lnx \implies \frac{dy}{dx}=\frac{1}{x} $

Some integral formulas:

1. $ \int x^n dx = \frac{x^{n+1}}{n+1} + C $ 

2. $ \int sinx dx = -cosx + C$

3. $ \int cosx dx = sinx + C $

4. $ \int tanx dx = log|sec x| + C$



Problem for Practice:

1. Find the equation of the line which is parallel to the given line $ y = 6x + 4 $ and passes through point (4, 6).

2. Find the  equation of the curve for which every point of the curve is at same distance from the point (3,2).

3. Differentiate the following with respect to x:

 (a) $ y = x^2 + 4x $ 

 (b) $z = 5x^3+10$

 (c) $y = sin4x + log|x|$

 (d) $y = sin^2x$

 (e)$ y = cos5x + tan2x + log|sin x| $

4. Integrate the following functions:

 (a) $y = sinx$

 (b)$y=5x^2 + 4x$

 (c) $y = sin^2x$

 (d) $ y = cos5x $

 (e)$y = logx $

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Thursday, 22 April 2021

Mathematics for Physics I

  April 22, 2021 Lakshman Jangid   Physics 11   No comments

 1. Algebra

Common Formulas:

1. $ (a+b)^2 = a^2+2ab+b^2 $

2. $ (a+b)^3 = a^3+b^3+3a^2b+3ab^2 $

3. $ (a^2-b^2)=(a+b)(a-b) $

4. $ (a+b+c)^2 = a^2+b^2+c^2+2ab+2bc+2ca $

5. $ (a+b)^2 + (a-b)^2 = 2(a^2+b^2) $

6. $ (a+b)^2 - (a-b)^2 = 4ab $

7. $ (a-b)^3 = a^3-b^3-3a^2b+3ab^2 $

Solving Quadratic Equation: Let any quadratic equation be $ ax^2+bx+c = 0 $. Roots of the equation are given by,  $x = \frac{-b \pm \sqrt{b^2-4ac}}{2a} $
If $ {b^2-4ac} = 0 $ then roots are real and equal.
If $ {b^2-4ac} > 0 $ then roots are distinct and real.
If $ {b^2-4ac} < 0 $ then roots are imaginary.
If $ \alpha $ and $ \beta $ are two roots of the equations, then  
Sum of roots: $ \alpha + \beta = \frac{-b}{a} $
Product of roots: $ \alpha \times \beta = \frac{c}{a} $
Difference of roots: $ \alpha - \beta = \frac{\sqrt{b^2 - 4ac}}{a} $

For example, Let $ x^2+x+1=0 $ is a quadratic equation and we need to find the roots of the equation.
For the given equation, $ b^2-4ac = 1 - (4 \times 1 \times 1) = 1-4 = -3  < 0 $
This means that the roots of the equation are imaginary. 
Roots will be, $ x = \frac{-1 \pm \sqrt{-3}}{2} = \frac{-1 - \sqrt{-3}}{2}, \frac{-1 + \sqrt{-3}}{2} $
For $ \sqrt{-1} = i $, then roots will be, \[x = \frac{-1 \pm \sqrt{-3}}{2} = \frac{-1 - \sqrt{3}i}{2}, \frac{-1 + \sqrt{3}i}{2}\]

Binomial Expansion:
If we need to expend $ (1+x)^n $ in powers of x where n is positive integer, we expand it binomially.
Expansion will be 
\[(1+x)^n = 1 + _{1}^{n}{x} + _{2}^{n}{x^2} + ....... + _{i}^{n}{x^i} + ..... + x^n \]
It can be written as \[(1+x)^n = \Sigma _{j=0}^{n} (_{j}^{n} C)(x^j)\]
where \[_{j}^{n} C = \frac{n!}{(n-j)! j!}, n! = n(n-1)(n-2).......3.2.1\] and $ 0! = 1 $.

The number of terms in the expansion of $ (1+x)^n $ are (n+1)

Binomial expansion for any index, i.e. if n is not a positive integer.
\[(1+x)^n = 1 + \frac{n}{1!}x + \frac{n(n-1)}{2!}x^2 + \frac{n(n-1)(n-2)}{3!}x^3 + .......... \infty terms\]

If |x| << 1 then $ (1+x)^n = 1 + nx $ i.e. we can ignore highest power of the expansion.

For example: Expand $ (1 + x ) ^ {-2} $.
$ (1+x)^{-2} = 1 + \frac{-2}{1!}x + \frac{-2(-2-1)}{2!}x^2 + \frac{-2(-2-1)(-2-2)}{3!}x^3 + .......... \infty = 1 -2x -3x^2 - 4x^3 + ......  $. 


Try Yourself:
Q1. Find the roots of the equations:
(a) $ x^2 + 2x + 3 = 0 $
(b) $ x^2 - 2x - 3 = 0 $
(c) $ x^2 + 30x  + 1 = 0 $
(d) $ 2x^2 + x + 1 = 0 $
 
Q2. Expand following:
(a) $ (1+x)^7 $
(b) $ (1+x)^{-7} $
(c) $ (1+y)^{-1} $
(d) $ (1+z)^{-10} $


***Solutions of the above problems will be uploaded soon..... 




2. Trigonometry

Relation between arc length, l, radius of the circle, r, and angle $ \theta $ subtended by the arc at the center, \[l = r \theta\]
 
Usefull Trigonometric Formulas for Right Angle Triangle 
Let any right angle triangle with Right angle at B, as shown in the figure click here to see large image. 






1. $ sin A = \frac{a}{b} $

2. $ cosA = \frac{c}{b} $

3. $ tanA = \frac{sin A}{cosA}=\frac{a}{c} $

4. $ cosecA = \frac{1}{sinA}=\frac{b}{a} $

5. $ secA = \frac{1}{cosA}= \frac{b}{c} $

6. $ cot A = \frac{1}{tanA}= \frac{cosA}{sinA}= \frac{c}{a}  $

7. $ sin^2 A + cos^2 A = 1 $ 

8. $ 1 + tan^2 A = sec^2 A $

9. $ 1+ cot^2 A = cosec^2 A $

Above formulas are valid only for Right angle triangle.

In general, for any triangle ABC where A, B and C are the angles, and a, b, and c are the sides opposite to angle A, B and C respectively. 
1. $ \frac{sinA}{a} = \frac{sinB}{b} = \frac{sinC}{c} $

2. $ cos A = \frac{b^2+c^2-a^2}{2bc} $ 

Value of some trigonometric functions:

 

 0

30        

45            

60 

90

 sin

 0  

 $ \frac{1}{2} $

 $ \frac{1}{\sqrt{2}}$

$ \frac{\sqrt{3}}{2}$ 

          1

cos 

 1 

  $ \frac{\sqrt{3}}{2}$

  $ \frac{1}{\sqrt{2}}$

 $ \frac{1}{2} $

         0

 tan

  0

 $\frac{1}{\sqrt{3}}$

1

 $ \sqrt{3} $

 $ \infty $


Compound Formula:

1. $ sin(A\pm B) = sinAcosB \pm sinBcosA $

2. $ cos(A\pm B) = cosAcosB \mp sinAsinB $

3. $ tan(A\pm B) = \frac{tanA\pm tanB}{1 \mp tanAtanB} $

4. $sin2A = 2sinAcosA $

5. $ cos2A = cos^2A - sin^2 A = 1 - 2sin^2 A = 2cos^2 A - 1 $

6. $tan2A = \frac{2tanA}{1-tan^2A} $

In the first quadrant, all trigonometric functions have positive values. In second quadrant, sine and cosec are positive and all others are negative. In third quadrant, tan and cot are positive and all others are negative. In fourth quadrant, cos and sec are positive and all other are negative.

1. $ sin(-\theta) = - sin \theta $

2. $ cos(-\theta) = cos \theta $

3. $ tan(-\theta) = - tan \theta $








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Friday, 25 December 2020

Ray optics: Prism and Optical Instruments

  December 25, 2020 Lakshman Jangid   Physics 12   No comments

1. Refraction through a prism is show in figure. After suffering refraction at two faces of a prism, the emergent ray is always found to bend towards the base of the prism. It is observed, that \[\angle A = \angle r_1 + \angle r_2\]and \[\angle A + \angle \delta = \angle i + \angle e\]Angle between the incident ray and the emergent ray i.e., $ \angle \delta $ is known as the angle of deviation. Its value depends upon the angle of incidence, refractive index of prism material and the angle of prism.

2. When refracted ray passes symmetrically through a prism i.e., when $ r_1 $ = $ r_2 $ and i = e, the light rays undergoes minimum deviation Dm and in such an eventuality, \[n_{21} = \frac{sin\frac{A+D_m}{2}}{sin{\frac{A}{2}}}\]where $ n_{21} $ is the refractive index of prism material with respect to the medium outside.

3. For a prism of small angle (i.e., if  $ \angle  A $ is small enough), the angle of deviation is given by \[\delta , D = (n_{21}-1)A\]

4. Dispersion is the phenomenon of splitting of light into its component colours (or wavelengths) on passing through a dispersive medium. The pattern of colour components of light is called its spectrum. For sunlight, the spectrum consists of seven constituent colours given by the acronym VIBGYOR. In white light spectrum the violet ray is deviated the most and the red ray is deviated the most and the red ray is deviated the least.

5. Cause of dispersion in variation of refractive index with wavelength of light. In fact, \[n = A + \frac{B}{\lambda ^2}\]where A and B are two constants are a given material. As a result, the refractive index of prism and consequently the angle of deviation is maximum for violet colour ray and least for red colour ray. It results in dispersion.

6. Angular dispersion produced by a prism for white light is difference in the angles of deviation of two extreme colours i.e., violet and red colours. Mathematically, Angular dispersion = $ \delta_v - \delta_r = (n_v - n_r)A $.

7. The light, while passing through earth’s atmosphere, gets scattered by the atmospheric particles. According to Rayleigh’s law of scattering, for scattering from tiny scattering objects e.g., air molecules the intensity of the light corresponding to a wavelength in the scattered light varies inversely as the fourth power of the wavelength. Mathematically, Amount of scattering $ \propto \frac{1}{\lambda^4} $

8. Blue colour of sky, blue colour of ocean water, reddish appearance of Sun at sunrise or sunset are some common phenomenon based on Rayleigh’s scattering. Due to this very reason, red light is used in danger signals.

9. Rainbow is an example of dispersion of light, caused by tiny water droplets hanging in the atmosphere after the rains.

10. The human eye is one of the most valuable and sensitive sense organ, the human being have. Our eyes have a lens system which focus the light rays coming from an object on the retina. Retina contains rods and cone which sense light intensity and colour respectively. Retina transmits electrical signals via the optic nerve to the brain, which analyses the information received and perceives the object.

11. The eyelens has the power of accommodation t adjust it focal length so as to focus objects situated at different distance form eye at the retina.

12. The least distance of distinct vision or near point of an eye is the minimum distance from the eye at which object can be seen distinctly. For a young adult with normal vision near point is at 25 cm.

13. The farthest point up to which an eye can see objects clearly is called the far point of eye. For a normal vision, the far point of eye lies at infinity. In this situation, our eye is least strained.

14. There are four common defects of vision. These are (i) myopia or short-sightedness (ii) hypermetropia or long-sightedness (iii) presbyopia and (iv) astigmatism.

15. A myopic eye can see near objects clearly but cannot see far off objects clearly i.e., the far point of defective eye is not at infinity but has shifted nearer to the eye. This defect may arise either due to (a) excessive curvature of the cornea, or (b) elongation of eyeball. The defect can be corrected by use of a concave (diverging) lens of appropriate power.

16. In hypermetropia, a person can see distance objects clearly but cannot see nearby objects distinctly i.e., for defective eye the near point has shifted away from the eye. This defect arises either due to less curvature of cornea or contraction of the eyeball. The defect can be corrected by use of convex (converging) lens of appropriate power. With increase in age the ciliary muscles gradually weaken and power of accommodation of eye decreases. It is called presbyopia. It can be corrected by using a converging lens for reading .

17. In astigmatism, a person cannot focus simultaneously on both horizontal and vertical lines. It arises when the cornea is not spherical in shape. The problem can be rectified by using cylindrical lens of desired radius of curvature with an appropriately directed axis.

18. A microscope is used for observing magnified images of nearby tiny objects. A simple magnifier or microscope is a convex lens of small focal length held near the object such that $ u \leq  f $.

19. In a simple microscope if image is formed at near point, the angular magnification of image is $ m = (1 + \frac{D}{f} ) $. However, if image is formed at infinity then magnification $ m = \frac{D}{f} $.

20. A compound microscope consists of two convex lenses, an objective lens of very small focal length ($ f_0 $) and small aperture and an eye lens of small focal length ($ f_e $) and slightly greater aperture, placed coaxially at a suitable fixed distance of distinct vision (D = 25 cm) from the eye and is virtual, inverted and highly magnified.

21. The angular magnification of a microscope is defined as the ratio of the angle subtended by the final image at the eye to the angle subtended by the object at the eye when seen directly. Angular magnification of a compound microscope is given by : 

(a) If final image is formed at near point of eye, then \[m = m_0 \times m_e = -\frac{v_0}{u_0}(1+\frac{D}{f_e})=-\frac{L}{f_0}(1+\frac{D}{f_e})\]

(b) If final image in a microscope is formed at infinity, then \[m =-\frac{L}{f_0}\frac{D}{f_e}\]

22. The resolving power of a compound microscope is its ability to show as distinct (separate), the images of two point objects lying close to each other. The limit of resolution of a microscope is measured by the minimum distance d between two point objects, whose images in microscope are seen as just separate. It is found that \[d = \frac{1.22 \lambda}{2nsin\alpha} = \frac{0.16 \lambda}{N.A.}\]where n = refractive index of medium between the object and the objective lens, $ 2\alpha $ = angle subtended by the diameter of objective lens at the focus point and N.A. = $ n sin \alpha $ = numerical aperture of objective. Resolving power of a microscope is the reciprocal of its limit of resolution. For higher resolving power the numerical aperture the numerical aperture of objective lens of microscope should be large and wavelength of light used should be as small as possible.

23. An astronomical telescope is used to form magnified and distinct images of heavenly bodies like planets stars, moons, galaxies etc. A refracting type astronomical telescope consists of a convex objective lens of large focal length and large aperture and another convex eyepiece lens of small total length and small aperture. Final image formed is inverted, magnified and at infinitly in normal adjustment.

24. The angular magnification of a telescope is defined as the ratio of the angle subtended at the eye by the final image to the angle subtended at the eye by the object directly. It is found that in normal adjustment \[m = -\frac{f_0}{f_e}\]and length of telescope tube $ L = f_0 + f_e $. 

25. In a reflecting type telescope we use a concave mirror (generally parabolic) of large aperture and large focal length as the objective and a convex lens of small focal length and aperture as the aberrations, are cheap, easy to construct and handle.

26. The limit of resolution of a telescope is measured by the angle ($ \Delta \theta $) subtended at its objective, by those two distant objects whose images are just seen separate through the telescope.

Resolving power of telescope = $ \frac{1}{\Delta \theta}= \frac{A}{1.22 \lambda}    $, where A is the aperture size of the telescope objective.

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Ray Optics: Reflection and Refraction

  December 25, 2020 Lakshman Jangid   Physics 12   No comments

1. Light is that form of energy which causes sensation of sight of your eyes. In fact, light is a part of electromagnetic radiation spectrum having its wavelength ranging from about 400 nm to 700nm.

2. In vacuum light of any wavelength (or any frequency) travels with a speed c = $ 2.99792458 \times 10^8 $ m/s but for ordinary calculations this value may be considered as c = $ 3 \times 10^8 $ m/s. The speed of light in vacuum is the highest speed attainable in nature. Moreover, speed of light in vacuum is independent of the relative motion between the source and the observer. No physical signal or message can travel with a speed greater than c.

3. As the wavelength of light is very small compared to the size of ordinary objects, a light wave can be considered to travel from one point to another point along a straight line path. Such a path is called a ray of light of right and a bundle of rays constitutes a beam of light.

4. In reflection of light, the light rays return to the same medium after striking the surface of another medium (say a mirror). The wavelength and the speed of light remains the same.

5. There are two basic laws of reflection, which are followed for every short of reflection. According to these

(i)  The incident ray, reflected ray and the normal at  the point of incidence all lie in the same plane.

(ii)  Angle of incidence (i) = angle of reflection (r).

6. For reflection from a plane mirror, the image formed is always erect, virtual and laterally inverted. The image is of exactly the same size as the object and the image is formed as such behind the mirror as the object is in front of it.

7. For a spherical mirror in the mid-point of reflecting surface is called its pole. The line passing through pole and the center of curvature of mirror is called its principle axis.

8. The principle focus of a spherical mirror is a point on its principle axis, where a beam of light incident parallel to principle axis of mirror, after reflection, actually converges to (in case of a concave mirror) or appears to diverge from (in case of a convex mirror). Distance of principle focus from pole is called the local length of given mirror.

9. Focal length of a spherical mirror is half of its radius of curvature i.e., f = R/2.

10. As per Cartesian sign convention system for mirrors, the light ray is taken to travel from left to right. All distances are measured from the pole as origin. The distance measured in the same direction as the incident light are taken as positive and those measured in the opposite direction are taken as negative. Thus, the distances to the right of pole will be + ve but distances to the left of pole will be – ve. Again distances above the principle axis are taken as + ve but distances below it – ve.

11. A concave mirror may form either a real or a virtual image depending upon the position of the object relative to the mirror. A convex mirror forms only virtual images.

12. If an object is placed at a distance u from the pole of a mirror of focal length f and its image is formed at a distance v from the pole, then according to mirror formula, we have \[\frac{1}{u} + \frac{1}{v}=\frac{1}{f}=\frac{2}{R}\].

13. If a thin linear object of height h is situated normally on principle axis of mirror at a distance u and its image of height h’ is formed at a distance v from the pole, then the linear magnification m is defined as  \[M = \frac{h'}{h} = -\frac{v}{u} = \frac{f}{f-u} = \frac{f-v}{f}\]-ve magnification means inverted image and +ve magnification means erect image.

14. When a light ray travels obliquely from one transparent medium to another, it changes the direction of its path at the interface of the two media. This is called “refraction” of light.

15. There are two laws of refraction, which are as follows:

(i)  The incident ray, the refracted ray and the normal to the interface at the point of incidence, all lie in the same plane.

(ii)    The ratio of the sine of the angle of incidence in 1st medium t sine the angle of refraction in second medium is a constant, knows as the refractive index of 2nd medium with respect to the 1st medium. Mathematically,  \[\frac{sin (i)}{sin (r)} = n_{21}\]Second law of refraction is known as Snell’s law.

16. Value of refractive index depends upon the pair of media and the wavelength of light but is independent of the angle of incidence.

17. When a light ray obliquely enters from an optically rarer medium to an optically denser medium, the light ray bends towards the normal. However, if a light ray travels from denser to rarer medium, it bends away from the normal.

18. Absolute refractive index of a transparent medium is defined as the ratio of the speed of light vacuum (c) to the speed of light in given medium (v) i.e., $ n = \frac{c}{v}$. It can be show that $ n_{21} = \frac{n_2}{n_1} = \frac{v_1}{ v_2} = \frac{\lambda_1}{\lambda_2}$. It is found that $n_{12} = \frac{1}{n_{21}} $.

19. When a light ray passes through a parallel sided slab of a transparent medium, the final emergent ray is parallel to the incident ray, but is laterally displaced by a distance d given by \[d = t \frac{sin (i – r)}{cos r}\]The value of lateral shift depends upon (a) thickness (t) of the transparent slab, (b) angle of incidence (i) and (c) refractive index of the material of slab.

20. When an object situated in medium number 2 is viewed from medium number 1, the apparent depth (height) of object appears to be different from its real depth 9height) and these are co-related as: \[\frac{d_{Real }}{ d_{Apparent}} = n_{12} = \frac{1}{n_{21}}\]

21. If an object situated in an optically denser medium is viewed by an observer situated in optically rarer medium, the apparent height is less than its real height. However, if an object situated in rarer medium is viewed by an observer situated in denser medium, then the apparent height is found to be more than its real height.

22. On account of atmospheric refraction the Sun is visible about 2 minutes before the actual sunrise and for 2 minutes even after the actual sunset. Thus, Sun also appear to be of oval shape at the time of sunrise or sunset on account of atmospheric refraction.

23. For a pair of media in contact, circuital angle is the angle of incidence in the denser medium corresponding to which angle of refraction in the rarer medium is 90 degree. If a light ray is incident on the surface of a rarer medium 2 from a denser medium 1, then \[Sin(i_c) = n_{21}\]Here $ n_{12}$ is the refractive index of 1st (denser) medium with respect to the 2nd (rarer) medium.

24. Total internal reflection is the phenomenon of complete reflection of light back into the denser medium, when a light ray coming from denser medium is incident on the surface of a rarer medium.Two essential conditions for total internal reflection are:

(i)  The light ray should travel in a denser medium towards a rarer medium.

(ii)  Angle of incidence in the denser medium should be greater than the critical angle for the pair of media in contact.

25. Values of critical angle of glass-air and water-air interfaces are 41.5 degree and 48.75 degree, respectively.

26. The brilliance of diamond, action of optical fibres and mirage etc., are the phenomena based on total internal reflection of light.

27. Prism make use for total internal reflection phenomenon to bend light by 90 degree or by 180 degree or to invert images without changing their size. Such prism have one angle 90 degree and the other two angles 45 degree each and are known as totally reflecting prisms or poroprisms.

28. For refraction at a single spherical surface, all distances are measured from the pole of the refracting surface. The distances measured in the direction fo incidence of light are taken as positive and the distances measured in the opposite direction are taken as negative. If object is considered to be situated on left side of pole,  then the sign convention agrees with the cartesian coordinate system. Accordingly, all distances on left side of pole are taken as negative and on right side of pole as positive. The height measured above the principle axis are taken as positive as heights measured downwards are taken as negative.

29. For refraction at a single spherical surface \[\frac{n_2}{v}-\frac{n_1}{u}=\frac{n_2 - n_1}{R}\]Where light beam is going from medium of refractive index n1 to medium of refractive index n2. The relation is true for concave as well as convex spherical surfaces and irrespective of the fact whether refraction is taking places from rarer medium to denser medium or vice-versa.

30. According of lens maker’s formula \[\frac{1}{f}=(n_{21}-1)(\frac{1}{R_1}-\frac{1}{R_2})\]Where $n_{21}$ is the refractive index of lens material w.r.t. the surrounding medium, $R_1$ and $R_2$ are the radii of curvature of two surfaces of lens and f its focal length.

31. For image formed by a thin lens, we have \[\frac{1}{v}-\frac{1}{u}=\frac{1}{f}\]All the above relation are the true for convex as well as concave surfaces/lenses and for real as well as virtual images.

32. Linear magnification (m) produced by a lens is defined as the ratio of the linear (lateral) size of the image to that of the object. Thus, \[m = \frac{h'}{h}=\frac{v}{u}=\frac{f-v}{f}=\frac{f}{f+u}\]For erect and virtual image, m is positive but for an inverted and real image, m is negative.

33. Power of lens is a measure of a degree of convergence or divergence of light incident on it. Mathematically, the power(p) of a lens is defined as the tangent of the angle by which it converges/ diverges a beam of light falling at unit distance from the optical centre. For a thin lens power is found to be the reciprocal of its focal length (f) i.e., \[P = \frac{1}{f}\]SI unit of power is dioptre (D).

34. Power of a converging (convex) lens is taken to be positive but that of a diverging (concave) less is taken negative.

35. For a combination of two (or more) thin lenses in contact, the effective focal length of the combination is given by \[\frac{1}{f} = \frac{1}{f_1}+\frac{1}{f_2}+......\]And in term of power, we have $ P = P_1 + P_2 + ...... $. 

36. For a combination of two or more lenses, the effective magnification for the combination is given by \[m = m_1 \times m_2 \times m_3 .......\]


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Thursday, 24 December 2020

Electromagnetic Waves

  December 24, 2020 Lakshman Jangid   Physics 12   No comments

1. A time-varying magnetic field gives rise to an electric field. Maxwell argued that a time-varying electric field should also give rise to a magnetic field. Maxwell thus tried to apply Ampere’s circuital law to find magnetic field outside a capacitor connected to a time-varying current. However, he noticed an inconsistency in Ampere’s circuital law.

2. To remove the inconsistency of Ampere’s circuital law, Maxwell suggested the existence of  "Displacement current”.

3. Displacement current ($ I_d$) is currents which come into play whenever the electric field and, consequently, the electric flux is changing with time. Mathematically, \[I_d = \epsilon_0 \frac{d\phi_E}{dt}\]

4. The sum of conduction current (I) and displacement current ($ I_d $) has the property of continuity along any closed path, although individually they may not be continuous. Thus, Maxwell modified Ampere’s circuital law as \[\oint \vec{B}.\vec{dl} = \mu_0 (I+I_d)\]With this modification the problem of inconsistency observed by Maxwell was rectified.

5. Maxwell was the first person who theoretically predicted the existence of electromagnetic waves, which are coupled with time-varying electric and magnetic fields propagating in space. The speed of these waves in free space is the same as that of light i.e. $ 3 \times 10^8 $ m/s.

6. Electromagnetic waves are produced by accelerated charges (or oscillating charge). An oscillating charge, which is an example of accelerating charge produces an oscillating electric field in space, which produces an oscillating magnetic field, which in turn is a source of oscillating electric field and so on. The oscillating electric filed and magnetic fields, thus, regenerate each other i.e., electromagnetic wave propagates through the space.

7. The frequency of the electromagnetic wave is same as the frequency of oscillation of the charge (electric field E) or the frequency of oscillating magnetic field (B).

8. Hertz was the first scientist to experimentally demonstrate the production of electromagnetic waves employing a crude form of an oscillatory LC circuit arrangement. Later on, Jagdish Chandra Bose produced electromagnetic waves of much shorter wavelengths. Marconi succeeded in transmitting electromagnetic waves over a distance of many kilometers.

9. Electromagnetic waves do not require any material medium for their propagation. In free space, their speed is given by \[c = \frac{1}{\sqrt{\mu_0 \epsilon_0}} = 3 \times 10^8\]In a medium of absolute permittivity (), the speed of electromagnetic waves is given by \[c = \frac{1}{\sqrt{\mu \epsilon}} = \frac{c}{\sqrt{K\mu_r}}\]

10. In an electromagnetic wave and electric and magnetic fields are in phase with each other. They attain their peak values at the same instant.

11. Electromagnetic waves are transverse in nature. The oscillating electric and magnetic fields are perpendicular to each other as well as perpendicular to the direction of propagation of the wave. In fact, the direction of ($ \vec{E}\times \vec{B} $) gives the direction of propagation of e.m. waves.

12. If we consider an electromagnetic wave propagating along positive x-axis then oscillating electric and magnetic fields may be represented as:\[\vec{E_y} = E_0sin(kx-\omega t)\hat{j}\] and \[\vec{B_z} = B_0sin(kx-\omega t)\hat{k}\]Here $\omega = 2\pi \nu $ is the angular frequency and $k = (\frac{2\pi}{\lambda})$ propagation constant of given electromagnetic wave.

13. In an electromagnetic wave, Amplitudes $E_0$ and $B_0$ of electric and magnetic fields in free space are related as: \[\frac{E_0}{B_0} = c\]

14. The energy density i.e., energy per unit volume of an electromagnetic wave consists of electric and magnetic contributions. Thus, The mean energy density \[U_m = U_E + U_B = \frac{1}{2}\epsilon_0 E^2_{rms} + \frac{1}{2\mu_0}B^2_{rms}\] It is found that average values of $ U_E $ and $ U_B $ are equal. 

15. Intensity of the electromagnetic wave is defined as the mean amount of energy passing through a unit area normally in unit time. It can be shown that Intensity \[I = U_m c = \frac{1}{2}\epsilon_0 c E^2_0 = \frac{c}{2\mu_0}B^2_0\]

16. The electromagnetic wave carries momentum too. If U be the total energy transferred to a surface by an electromagnetic wave in time t, then momentum delivered to this surface, assuming the surface to be completely absorbent, is \[p = \frac{U}{c}\]The average force exerted by e.m. wave on the surface will be \[F= \frac{p}{t} = \frac{U}{ct}\]

17. The classification of electromagnetic radiation waves according to frequency is known as “electromagnetic spectrum”. There is no sharp division between one kind of wave and the next and the classification is based roughly on how the waves are produced/ detected.

18. Complete electromagnetic spectrum in ascending order of frequency (or in decreasing order of wavelength) broadly consists of seven parts namely 

(i) Radio waves, (ii) Microwaves (iii) Infrared waves, (iv) Visible light rays, (v) Ultraviolet rays, (vi) X-rays, and (vii) Gamma rays.

19. Radio waves are produced by accelerated motion of charges in conducting wires and are used in radio and TV communication. They are in the frequency range of 500kHz to about 1000 MHz (or 1 GHz). These are further subdivided as a medium band, short band, HF band, VHF band, UHF band, etc.

20. Microwaves are extremely short-wavelength radio waves having a frequency range of $ 10^9 $ Hz to about 10 11 Hz and are produced by special vacuum tubes e.g., klystrons, magnetrons, and Gunn diodes. These are used in radar, microwave telecommunication, microwave oven, etc.

21. Inferred waves are produced by hot bodies and molecules and are characterized by their heating property. Inferred radiation plays an important role in maintaining the earth’s warmth by the greenhouse effect. Inferred rays are widely used in the remote switches of household electronic systems such as TV sets, video recorders, hi-fi systems, etc.

22. Visible parts are that part of the electromagnetic spectrum which is detected by the human eye. It runs from about $ 4 \times 10^{14} $ Hz to $ 7 \times 10^{14} $ Hz. Visible light emitted or reflected from objects around us provides us information about the world.

23. Ultraviolet rays consist of radiation in the frequency range $ 7 \times 10^{14} $Hz to $ 5 \times  10^{17} $ Hz (or wavelength range from 400 nm to 0.6 nm). These are produced by the sun, special lamps like mercury lamp, hydrogen tube etc, and very hot bodies. Ultraviolet rays have various uses such as in  LASIK eye surgery, to kill germs in water purifiers, as a disinfectant in hospitals, etc. however, ultraviolet light in large quantities has harmful effects on humans.

24. Ozone layer present in the atmosphere at an altitude of about 40 – 50 km absorbs most of the ultraviolet rays coming from the sun and thus, form a protective ring around the earth.

25. X-rays cover wavelengths from about 1 nm to $10^{-3} $ nm. These are produced by bombarding high energy electrons on a metal target. X-rays are used as a diagnostic tool in medicine, as a treatment for certain forms of cancer, and for scientific research.

26. Gamma rays are the hardest electromagnetic waves having wavelengths even less than $ 10^{-3} $ nm. These are produced in nuclear reactions and are also emitted during radioactive decay of the nuclei. These are used in medicine for destroying cancer cells.


Electromagnetic Spectrum

 Type                            

Wavelength range 

 Production

 Detection

 Radio

 > 0.1 m

 Rapid acceleration and decelerations of electrons in aerials

 Reciever's aerial

 Microwave

 0.1 m to 1 mm

 Klystron valve or magnetron valve

 Point contact diode

 Infrared

 1 mm to 700 nm

 Vibration of atoms and molecules

 Thermopiles, Bolometer, Infrared photographic film

 Light

 700 nm to 400 nm

 Electrons in atom emit light when they move from one energy level to a lower energy level

 The eye Photocells, Photographic film

 Ultraviolet

 400 nm to 1 nm

 Inner shell electrons in atoms moving from one energy level to lower level 

 Photocells, Photographic film

 X-ray

 1 nm to $10^{-3}$ nm 

 X-ray tubes or inner shell electrons 

 Photographic film, Geiger tubes, Ionisation chamber

 Gamma Ray

 < $ 10^{-3} $ nm

 Radioactive decay of the nucleus

- do -


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