1. Capacitance of a parallel capacitor, V = 2 F Distance between the two plates, d = 0.5 cm = 0.5 x 10-2 m Capacitance of a parallel plate capacitor is given by the relation, C= ε0A/d A =Cd/ε0 Where, ε0 = Permittivity of free space Therefore A= 2x 0.5 x 10⁻²)/(8.85 x 10⁻¹²) Therefore, A = 1130 km² HencRead more

    Capacitance of a parallel capacitor, V = 2 F

    Distance between the two plates, d = 0.5 cm = 0.5 x 10-2 m

    Capacitance of a parallel plate capacitor is given by the relation,

    C= ε0A/d

    A =Cd/ε0

    Where,

    ε0 = Permittivity of free space

    Therefore A= 2x 0.5 x 10⁻²)/(8.85 x 10⁻¹²)

    Therefore, A = 1130 km²

    Hence, the area of the plates is too large.

    To avoid this situation, the capacitance is taken in the range of μF.

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  2. Total required capacitance, C = 2 pF Potential difference, V = 1, kV = 1000 V Capacitance of each capacitor, C₁ = lμF Each capacitor can withstand a potential difference, V₁= 400 V Suppose a number of capacitors are connected in series and these series circuits are connected in parallel (row) to eacRead more

    Total required capacitance, C = 2 pF Potential difference, V = 1, kV = 1000 V

    Capacitance of each capacitor, C₁ = lμF

    Each capacitor can withstand a potential difference, V₁= 400 V

    Suppose a number of capacitors are connected in series and these series circuits are connected in parallel (row) to each other. The potential difference across each row must be 1000 V and potential difference across each capacitor must be 400 V.

    Hence, number of capacitors in each row is given as 1000/4 = 2.5

    Hence, there are three capacitors in each row.

    Capacitance of each row = 1/(1+1+1) = 1/3 μF

    Let there are n rows, each having three capacitors, which are connected in parallel. Hence, equivalent capacitance of the circuit is given as

    1/3 +1/3 + 1/3 +……..n terms = n/3

    However, capacitance of the circuit is given as 2 μF.

    Therefore n/3 =2 ,therefore n=6

    Hence, 6 rows of three capacitors are present in the circuit. A minimum of 6 x3 i.e.,18 capacitors are required for the given arrangement.

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  3. Ans (a). Zero at both the points Charge - q is located at (0, 0, — a) and charge + q is located at (0, 0, a). Hence, they form a dipole. Point (0, 0, z) is on the axis of this dipole and point (x, y, 0) is normal to the axis of the dipole. Hence, electrostatic potential at point (x, y, 0) is zero. ERead more

    Ans (a).

    Zero at both the points

    Charge – q is located at (0, 0, — a) and charge + q is located at (0, 0, a). Hence, they form a dipole. Point (0, 0, z) is on the axis of this dipole and point (x, y, 0) is normal to the axis of the dipole. Hence, electrostatic potential at point (x, y, 0) is zero. Electrostatic potential at point (0, 0, z) is given by,

    V= (1/4π ε0 ) [q/(z-a)] + (1/4π ε0 ) [-q/(z+a)]

    = q (z+a -z + a )/ [4π ε0 (z²-a²)]

    =2qa/[4π ε0 (z²-a²)]

    =p/[4π ε0 (z²-a²)]

    Where,

    ε0 = Permittivity of free space and p = Dipole moment of the system of two charges = 2qa

    Ans (b).

    Distance r is much greater than half of the distance between the two charges.

    Hence, the potential (V) at a distance r is inversely proportional to square of the distance,

    i.e. V ∝ 1/r²

    Ans (c).

    Zero

    The answer does not change if the path of the test is not along the x-axis.

    A test charge is moved from point (5, 0, 0) to point (-7, 0, 0) along the x-axis.

    Electrostatic potential (V₁) at point (5, 0, 0) is given by,

    V₁= -(q /4π ε0) 1/[√(5-0)²+ (-a)²]     + (q /4π ε0) 1/[√(5-0)²+ (a)²]

    =  -(q /4π ε0) 1/[√25+ a²]                  + (q /4π ε0) 1/[√25+ a²]

    = 0

    Electrostatic potential ,V₂ at point (-7,0,0) is given by

    V₁= -(q /4π ε0) 1/[√(7-0)²+ (-a)²]     + (q /4π ε0) 1/[√(7-0)²+ (a)²]

    =  -(q /4π ε0) 1/[√49+ a²]                 + (q /4π ε0) 1/[√49+ a²]

    = 0

    Hence, no work is done in moving a small test charge from point (5, 0, 0) to point (-7, 0, 0) along the x- axis.

    The answer does not change because work done by the electrostatic field in moving a test charge between the two points is independent of the path connecting the two points.

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  4. Let a be the radius of a sphere A, QA be the charge on the sphere, and CA be the capacitance of the sphere. Let b be the radius of a sphere B, QB be the charge on the sphere, and CB be the capacitance of the sphere. Since the two spheres are connected with a wire, their potential (V) will become equRead more

    Let a be the radius of a sphere A, QA be the charge on the sphere, and CA be the capacitance of the sphere.

    Let b be the radius of a sphere B, QB be the charge on the sphere, and CB be the capacitance of the sphere.

    Since the two spheres are connected with a wire, their potential (V) will become equal.

    Let EA be the electric field of sphere A and EB be the electric field of sphere B. Therefore, their ratio,

    EA/E= (QA /4π ε0 a2 ) x (b2 ε0 )/QB

    EA/E= (QA / QB) x (b2 / a2 )  ———————-Eq-1

    However , QA / Q=CAV/ CV

    and  CA/ C=a/b

    Therefore  QA / Q=a/b  ———————-Eq-2

    Putting the values of Eq-2 in Eq-1 ,we obtain

    EA/E= (a/b ) x (b2 / a2 )=b/a

    Therefore ,the ratio of electric fields at the surface is b/a.

     

     

     

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  5. The distance between electron-proton of a hydrogen atom, d = 0.53 A Charge on an electron, q₁ = -1.6 x 10-19 C Charge on a proton, q2 = +1.6 x 10-19 C Ans (a). Potential at infinity is zero. Potential energy of the system, p-e = Potential energy at infinity - Potential energy at distance, d = 0 - (qRead more

    The distance between electron-proton of a hydrogen atom, d = 0.53 A

    Charge on an electron, q₁ = -1.6 x 10-19 C Charge on a proton, q2 = +1.6 x 10-19 C

    Ans (a).

    Potential at infinity is zero.

    Potential energy of the system, p-e

    = Potential energy at infinity – Potential energy at distance, d

    = 0 – (q₁-q₂)/4πε0 d

    Where, ε0 is the permittivity of free space and

    1/4πε0 =9x 10⁹ Nm²C⁻²

    Therefore Potential Energy = 0- (9x 10⁹) x (1.6 x 10⁻¹⁹)² /(0.53 x 10¹⁰)

    = -43.7x 10⁻¹⁹ J , (Since 1.6 x 10⁻¹⁹ J = 1 eV)

    Therefore  Potential energy =-43.7×10⁻¹⁹ = -(43.7 x 10⁻¹⁹)/(1.6 x 10⁻¹⁹) =-27.2 eV

    Therefore, the potential energy of the system is -27.2 eV.

    Ans (b).

    Kinetic energy is half of the magnitude of potential energy.

    Kinetic energy = 1/2 x(-27.2) = 13.6 eV

    Total energy = 13.6 – 27.2 = 13.6 eV

    Therefore, the minimum work required to free the electron is 13.6 eV.

    Ans (c).

    When zero of potential energy is taken, d = 1.06 A

    Therefore Potential energy of the system = Potential energy at d₁- Potential energy at d

    = (q₁q₂)/4πε0 d₁   –   27.2 eV

    = (9 x 10⁹) x (1.6 x 10⁻¹⁹)²  / ( 1.06 x 10⁻¹⁰)   -27.2 eV

    =21.73 x 10⁻¹⁹ J – 27.2 eV =

    =13.58 eV – 27.2 eV= – 13.6 eV

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