
Drift velocity of charge carriers in a conductor refers to the average velocity that these carriers, such as electrons, attain due to an electric field applied across the conductor. When an electric field is applied, it causes the charge carriers to move in a particular direction, resulting in a net flow of charge, which is what we observe as electric current.
The relationship between drift velocity (v_d) and the current (I) flowing through a conductor can be expressed by the equation:
- I = nAv_dq
Where:
- I is the electric current.
- n is the number density of charge carriers (number of charge carriers per unit volume).
- A is the cross-sectional area of the conductor.
- v_d is the drift velocity.
- q is the charge of each carrier.
This equation indicates that the current is directly proportional to the drift velocity, meaning that as the drift velocity increases, the current also increases, assuming that the number density of charge carriers and the cross-sectional area remain constant.
Drift velocity of charge carriers in a conductor refers to the average velocity that these carriers, such as electrons, attain due to an electric field applied across the conductor. When an electric field is applied, it causes the charge carriers to move in a particular direction, resulting in a net flow of charge, which is what we observe as electric current.
The relationship between drift velocity (v_d) and the current (I) flowing through a conductor can be expressed by the equation:
- I = nAv_dq
Where:
- I is the electric current.
- n is the number density of charge carriers (number of charge carriers per unit volume).
- A is the cross-sectional area of the conductor.
- v_d is the drift velocity.
- q is the charge of each carrier.
This equation indicates that the current is directly proportional to the drift velocity, meaning that as the drift velocity increases, the current also increases, assuming that the number density of charge carriers and the cross-sectional area remain constant.




