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A current of 4 A is flowing in a cylindr...

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

A

`2 * 10^(19)`

B

`3 * 10^(20)`

C

`2.5 * 10^(19)`

D

`4 * 10^(18)`

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To find the number of free electrons passing per second through the cross-section of a cylindrical conductor with a current of 4 A, we can follow these steps: ### Step 1: Understand the relationship between current, charge, and time The current (I) flowing through a conductor is defined as the rate of flow of charge (Q) per unit time (T). Mathematically, this is expressed as: \[ I = \frac{dQ}{dT} \] ### Step 2: Rearrange the formula to find charge From the above equation, we can express the total charge (Q) that flows in a given time (T): \[ Q = I \times T \] ### Step 3: Substitute the known values In this case, we have: - Current (I) = 4 A - Time (T) = 1 second (since we want the number of electrons per second) Substituting these values into the equation gives: \[ Q = 4 \, \text{A} \times 1 \, \text{s} = 4 \, \text{C} \] ### Step 4: Relate charge to the number of electrons The total charge (Q) can also be expressed in terms of the number of electrons (n) and the charge of a single electron (e): \[ Q = n \times e \] where the charge of a single electron \( e \) is approximately \( 1.6 \times 10^{-19} \, \text{C} \). ### Step 5: Rearrange to find the number of electrons We can rearrange the equation to solve for the number of electrons (n): \[ n = \frac{Q}{e} \] ### Step 6: Substitute the values to find n Substituting the values we have: \[ n = \frac{4 \, \text{C}}{1.6 \times 10^{-19} \, \text{C}} \] ### Step 7: Calculate the number of electrons Calculating this gives: \[ n = \frac{4}{1.6 \times 10^{-19}} = 2.5 \times 10^{19} \, \text{electrons per second} \] ### Conclusion Thus, the number of free electrons passing per second through the cross-section of the conductor is: \[ n = 2.5 \times 10^{19} \, \text{electrons/second} \]
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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 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

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