To address the question, we need to understand the behavior of free electrons in a conductor when subjected to an electric field.
- Free Electrons: In a conductor, free electrons are those that are not bound to a particular atom and can move freely through the material. These electrons are responsible for the flow of current when an electric field is applied.
- Drift Velocity: When an electric field is applied across a conductor, the free electrons experience a force that causes them to drift towards the higher potential. This movement of electrons is called the "drift velocity" and is generally very slow compared to the speed of the individual random motion of the electrons.
- Electric Potential: The electric potential is higher at the end of the conductor where the electric field is applied. Electrons, being negatively charged, move from regions of lower potential to higher potential under the influence of the electric field.
- While electrons drift from lower to higher potential, not all free electrons in the conductor are moving in the same direction at any given instant. The reason for this is the nature of the random thermal motion of the electrons. Each electron has its own random motion due to its thermal energy, which is much faster than the drift motion caused by the electric field.
- The overall drift velocity, which is the net movement of electrons due to the applied electric field, is very small and is in the direction from lower to higher potential (opposite to the electric field). However, the individual electrons still undergo random motion in all directions, which results in a random distribution of velocities.
No, not all the free electrons move in the same direction. The electrons experience random motion due to thermal energy, but they drift overall in the direction opposite to the electric field due to the applied potential difference.
While electrons drift in the direction from lower to higher potential, their random thermal motion means that not all of the free electrons are moving in the same direction at any given moment.
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.


For the circuit shown above, the equivalent gate is:
Alexia Limited invited applications for issuing 1,00,000 equity shares of ₹ 10 each at premium of ₹ 10 per share.
The amount was payable as follows:
Applications were received for 1,50,000 equity shares and allotment was made to the applicants as follows:
Category A: Applicants for 90,000 shares were allotted 70,000 shares.
Category B: Applicants for 60,000 shares were allotted 30,000 shares.
Excess money received on application was adjusted towards allotment and first and final call.
Shekhar, who had applied for 1200 shares failed to pay the first and final call. Shekhar belonged to category B.
Pass necessary journal entries for the above transactions in the books of Alexia Limited. Open calls in arrears and calls in advance account, wherever necessary.
