Home
Class 12
PHYSICS
A conductor has been given a charge -3 x...

A conductor has been given a charge `-3 xx 10^(-7) C` by transferring electron. Mass increase (in kg) of the conductor and the number of electrons added to the conductor are respectively

A

`2 xx 10^(-16)` and `2 xx 10^(31)`

B

`5 xx 10^(-31)` and `5 xx 10^(19)`

C

`3 xx 10^(-19)` and `9 xx 10^(16)`

D

`2 xx 10^(-18)` and `2 xx 10^(12)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to determine two things: the number of electrons added to the conductor and the increase in mass of the conductor due to these electrons. ### Step 1: Calculate the number of electrons added We know that the charge \( Q \) on the conductor is given by the formula: \[ Q = N \cdot e \] where: - \( Q \) is the total charge, - \( N \) is the number of electrons, - \( e \) is the charge of one electron, which is approximately \( 1.6 \times 10^{-19} \) coulombs. Given that the charge on the conductor is \( -3 \times 10^{-7} \) coulombs, we can rearrange the formula to find \( N \): \[ N = \frac{Q}{e} \] Substituting the values: \[ N = \frac{-3 \times 10^{-7}}{-1.6 \times 10^{-19}} \] Calculating this gives: \[ N = \frac{3 \times 10^{-7}}{1.6 \times 10^{-19}} \approx 1.875 \times 10^{12} \] This can be approximated to: \[ N \approx 2 \times 10^{12} \] ### Step 2: Calculate the increase in mass of the conductor The increase in mass \( \Delta M \) of the conductor due to the added electrons can be calculated using the formula: \[ \Delta M = N \cdot m_e \] where: - \( m_e \) is the mass of one electron, approximately \( 9.1 \times 10^{-31} \) kg. Substituting the values we found: \[ \Delta M = 2 \times 10^{12} \cdot 9.1 \times 10^{-31} \] Calculating this gives: \[ \Delta M \approx 1.82 \times 10^{-18} \text{ kg} \] This can be approximated to: \[ \Delta M \approx 2 \times 10^{-18} \text{ kg} \] ### Final Answers - The number of electrons added to the conductor: \( 2 \times 10^{12} \) - The increase in mass of the conductor: \( 2 \times 10^{-18} \text{ kg} \)
Doubtnut Promotions Banner Mobile Dark
|

Topper's Solved these Questions

  • ELECTROSTATICS

    DC PANDEY ENGLISH|Exercise Assertion and Reason|15 Videos
  • ELECTROSTATICS

    DC PANDEY ENGLISH|Exercise Match the columns|5 Videos
  • ELECTROSTATICS

    DC PANDEY ENGLISH|Exercise Check point 1.5|20 Videos
  • ELECTROSTATIC POTENTIAL AND CAPACITORS

    DC PANDEY ENGLISH|Exercise (C) Chapter exercises|50 Videos
  • GRAVITATION

    DC PANDEY ENGLISH|Exercise All Questions|135 Videos

Similar Questions

Explore conceptually related problems

A current of 4.8 A is flowing in a conductor the number of electrons passing per sec through the conductor will be

A substance with less number of free electrons is said to be good conductor.

Knowledge Check

  • A metallic sphere of radius 18 cm has been given a charge of 5xx10^(-6)C. The energy of the charged conductor is

    A
    `0.2J`
    B
    `0.6J`
    C
    `1.2J`
    D
    `2.4J`
  • Similar Questions

    Explore conceptually related problems

    In a metal in the solid state, such as a copper wire, the atoms are strongly bound to one another and occupý fixed positions. Some electrons (called the conductor electrons) are free to move in the body of the metal while the other are strongly bound to their atoms. In good conductors, the number of free electrons is very large of the order of 10^(28) electrons per cubic metre in copper. The free electrons are in random motion and keep colliding with atoms. At room temperature, they move with velocities of the order of 10^5 m/s. These velocities are completely random and there is not net flow of charge in any directions. If a potential difference is maintained between the ends of the metal wire (by connecting it across a battery), an electric field is set up which accelerates the free electrons: These accelerated electrons frequently collide with the atoms of the conductor, as a result, they acquire a constant speed called the drift speed which is given by V_e = 1/enA where I = current in the conductor due to drifting electrons, e = charge of electron, n = number of free electrons per unit volume of the conductor and A = area of cross-section of the conductor. The drift speed of free electrons in a conductor depends upon

    In a metal in the solid state, such as a copper wire, the atoms are strongly bound to one another and occupý fixed positions. Some electrons (called the conductor electrons) are free to move in the body of the metal while the other are strongly bound to their atoms. In good conductors, the number of free electrons is very large of the order of 10^(28) electrons per cubic metre in copper. The free electrons are in random motion and keep colliding with atoms. At room temperature, they move with velocities of the order of 10^5 m/s. These velocities are completely random and there is not net flow of charge in any directions. If a potential difference is maintained between the ends of the metal wire (by connecting it across a battery), an electric field is set up which accelerates the free electrons: These accelerated electrons frequently collide with the atoms of the conductor, as a result, they acquire a constant speed called the drift speed which is given by V_e = 1/enA where I = current in the conductor due to drifting electrons, e = charge of electron, n = number of free electrons per unit volume of the conductor and A = area of cross-section of the conductor. If no potential difference is maintained between the ends of a conductor

    In a metal in the solid state, such as a copper wire, the atoms are strongly bound to one another and occupý fixed positions. Some electrons (called the conductor electrons) are free to move in the body of the metal while the other are strongly bound to their atoms. In good conductors, the number of free electrons is very large of the order of 10^(28) electrons per cubic metre in copper. The free electrons are in random motion and keep colliding with atoms. At room temperature, they move with velocities of the order of 10^5 m/s. These velocities are completely random and there is not net flow of charge in any directions. If a potential difference is maintained between the ends of the metal wire (by connecting it across a battery), an electric field is set up which accelerates the free electrons: These accelerated electrons frequently collide with the atoms of the conductor, as a result, they acquire a constant speed called the drift speed which is given by V_e = 1/enA where I = current in the conductor due to drifting electrons, e = charge of electron, n = number of free electrons per unit volume of the conductor and A = area of cross-section of the conductor. A current of 1 A flows through a copper wire. The number of electrons passing through any cross-section of the wire in 1.6 sec is (charge of a electron = 1.6 xx 10^(-19 c) .

    In a metal in the solid state, such as a copper wire, the atoms are strongly bound to one another and occupý fixed positions. Some electrons (called the conductor electrons) are free to move in the body of the metal while the other are strongly bound to their atoms. In good conductors, the number of free electrons is very large of the order of 10^(28) electrons per cubic metre in copper. The free electrons are in random motion and keep colliding with atoms. At room temperature, they move with velocities of the order of 10^5 m/s. These velocities are completely random and there is not net flow of charge in any directions. If a potential difference is maintained between the ends of the metal wire (by connecting it across a battery), an electric field is set up which accelerates the free electrons: These accelerated electrons frequently collide with the atoms of the conductor, as a result, they acquire a constant speed called the drift speed which is given by V_e = 1/enA where I = current in the conductor due to drifting electrons, e = charge of electron, n = number of free electrons per unit volume of the conductor and A = area of cross-section of the conductor. A constant potential difference is maintained between the ends of a conductor having nonuniform cross-section. Which of the following quantities will not change along the length of the conductor

    In a metal in the solid state, such as a copper wire, the atoms are strongly bound to one another and occupý fixed positions. Some electrons (called the conductor electrons) are free to move in the body of the metal while the other are strongly bound to their atoms. In good conductors, the number of free electrons is very large of the order of 10^(28) electrons per cubic metre in copper. The free electrons are in random motion and keep colliding with atoms. At room temperature, they move with velocities of the order of 10^5 m/s. These velocities are completely random and there is not net flow of charge in any directions. If a potential difference is maintained between the ends of the metal wire (by connecting it across a battery), an electric field is set up which accelerates the free electrons: These accelerated electrons frequently collide with the atoms of the conductor, as a result, they acquire a constant speed called the drift speed which is given by V_e = 1/enA where I = current in the conductor due to drifting electrons, e = charge of electron, n = number of free electrons per unit volume of the conductor and A = area of cross-section of the conductor. A uniform wire of length 2.0 m and cross-sectional area 10^(-7) m^(2) carries a current of 1.6 A. If there are 10^(28) free electrons per m in copper, the drift speed of electrons in copper is

    Consider a conductor of length 40 cm where a potential difference of 10V is maintained between the ends of the conductor. Find the mobility of the electrons provided the drift velocity of the electrons is 5xx10^(-6) ms^(-1)

    A current of 4 A is flowing in a cylindrical conductor. The number of free electrons passing per second through the cross-section of conductor is