1. Ans (a). Long distance radio broadcasts use shortwave bands because only these bands can be refracted by the ionosphere. Ans (b). It is necessary to use satellites for long distance TV transmissions because television signals are of high frequencies and high energies. Thus, these signals are not refRead more

    Ans (a).

    Long distance radio broadcasts use shortwave bands because only these bands can be refracted by the ionosphere.

    Ans (b).

    It is necessary to use satellites for long distance TV transmissions because television signals are of high frequencies and high energies. Thus, these signals are not reflected by the ionosphere. Hence, satellites are helpful in reflecting TV signals. Also, they help in long distance TV transmissions.

    Ans (c).

    With reference to X-ray astronomy, X-rays are absorbed by the atmosphere. However, visible and radio waves can penetrate it. Hence, optical and radio telescopes are built on the ground, while X-ray astronomy is possible only with the help of satellites orbiting the Earth, (d) The small ozone layer on the top of the atmosphere is crucial for human survival because it absorbs harmful ultraviolet radiations present in sunlight and prevents it from reaching the Earth’s surface.

    Ans (d).

    In the absence of an atmosphere, there would be no greenhouse effect on the surface of the Earth. As a result, the temperature of the Earth would decrease rapidly, making it chilly and difficult for human survival.

    Ans (e).

    A global nuclear war on the surface of the Earth would have disastrous consequences.

    Post-nuclear war, the Earth will experience severe winter as the war will produce clouds of smoke that would cover maximum parts of the sky, thereby preventing solar light form reaching the atmosphere. Also, it will lead to the depletion of the ozone layer.

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  2. Ans (a). Radio waves; it belongs to the short wavelength end of the electromagnetic spectrum. Ans (b). Radio waves; it belongs to the short wavelength end. Ans (c). Temperature, T = 2.7 °K , λmis given by Planck's law as: λm = 0.29/2.7= 0.11 cm This wavelength corresponds to microwaves. Ans (d). ThiRead more

    Ans (a).

    Radio waves; it belongs to the short wavelength end of the electromagnetic spectrum.

    Ans (b).

    Radio waves; it belongs to the short wavelength end.

    Ans (c).

    Temperature, T = 2.7 °K , λmis given by Planck’s law as:

    λm = 0.29/2.7= 0.11 cm

    This wavelength corresponds to microwaves.

    Ans (d).

    This is the yellow light of the visible spectrum.

    Ans (e).

    Transition energy is given by the relation,

    E = hν, Where, h = Planck’s constant = 6.6 x 10-34 Js,

    ν = Frequency of radiation

    Energy, E = 14.4 K eV

    Therefore ,  ν = E/h

    =(14.4 x 10³ x 1.6 x 10⁻¹⁹)/( 6.6 x 10-34 )

    =3.4 x 10¹⁸Hz

    This corresponds to X-rays.

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  3. A body at a particular temperature produces a continuous spectrum of wavelengths. In case of a black body, the wavelength corresponding to maximum intensity of radiation is given according to Planck's law. It can be given by the relation, λm= 0.29/T cm K Where, λm= maximum wavelength and T = temperaRead more

    A body at a particular temperature produces a continuous spectrum of wavelengths. In case of a black body, the wavelength corresponding to maximum intensity of radiation is given according to Planck’s law. It can be given by the relation,

    λm= 0.29/T cm K

    Where,

    λm= maximum wavelength and T = temperature.

    Thus, the temperature for different wavelengths can be obtained as:

    For   λ= 10⁻4 cm; T = 0.29/10⁻4 = 2900 °K

    For  λm = 5 x 10⁻5 cm; T = 0.29/(5 x 10⁻5) = 5800 °K

    For  λm =  10⁻⁶ cm; T = 0.29/( 10⁻⁶) = 290000 °K and so on.

    The numbers obtained tell us that temperature ranges are required for obtaining radiations in different parts of an electromagnetic spectrum. As the wavelength decreases, the corresponding temperature increases.

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  4. Power rating of bulb, P = 100 W It is given that about 5% of its power is converted into visible radiation. Therefore ,Power of visible radiation, P' = (5/100 ) x 100 = 5 W Hence, the power of visible radiation is 5W. Ans (a). Distance of a point from the bulb, d = 1 m Hence, intensity of radiationRead more

    Power rating of bulb, P = 100 W

    It is given that about 5% of its power is converted into visible radiation.

    Therefore ,Power of visible radiation,

    P’ = (5/100 ) x 100 = 5 W

    Hence, the power of visible radiation is 5W.

    Ans (a).

    Distance of a point from the bulb, d = 1 m Hence, intensity of radiation at that point is given as:

    I = P’/(4πd²) =5/4π(1)² =0.398 W/m²

    Ans (b).

    Distance of a point from the bulb, d1 = 10 m Hence, intensity of radiation at that point is given as:

    I = P’/[4π(d1)²]

    =5/4π(10)² =0.00398 W/m²

     

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  5. Ans (a). From the given electric field vector, it can be inferred that the electric field is directed along the negative x direction. Hence, the direction of motion is along the negative y direction i.e. —J. Ans (b). It is given that, E = 3.1 N/C cos[(l.8 rad/m)y+(5.4 x 10⁸ rad/s)t]i --------------ERead more

    Ans (a).

    From the given electric field vector, it can be inferred that the electric field is directed along the negative x direction. Hence, the direction of motion is along the negative y direction i.e. —J.

    Ans (b).

    It is given that,

    E = 3.1 N/C cos[(l.8 rad/m)y+(5.4 x 10⁸ rad/s)t]i ————–Eq-1

    The general equation for the electric field vector in the positive x direction can be written as:

    E= E0 sin (kx -ωt) i—————————————-Eq-2

    On comparing equations (1) and (2), we get Electric field amplitude, Eo = 3.1 N/C Angular frequency, ω = 5.4 x 108 rad/s

    Wave number, k = 1.8 rad/m

    Wavelength, λ = 2π/1.8 = 3.490 m

    Ans (c).

    Frequency of wave is given as:

    ν =  ω /2π = (5.4 x 108)/2π =8.6 x 10⁷ Hz

    Ans (d).

    Magnetic field strength is given as:

    B0= E0/c

    Where, c = Speed of light = 3 x 108 m/s

    Therefore, B0= 3.1/(3 x 108 )= 1.03 x 10⁻⁷T

    Ans (e).

    On observing the given vector field, it can be observed that the magnetic field vector is directed along the negative z direction. Hence, the general equation for the magnetic field vector is written as:

    B= B0 cos (ky + ωt)k

    = {(1.03 x10⁻7 T)cos[(1.8 rad/m)y+(5.4 x 106 rad/s)t ]}k

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