Concept:
In a conductor, free electrons move randomly due to thermal energy.
When an electric field is applied, these electrons acquire a small net velocity in a particular direction.
This average velocity is called
drift velocity.
Definition:
Drift velocity is the average velocity acquired by charge carriers in a conductor under the influence of an external electric field.
It is denoted by \( v_d \).
Step 1: Motion of Charge Carriers
Consider:
- A conductor of cross-sectional area \( A \)
- Number of charge carriers per unit volume = \( n \)
- Charge of each carrier = \( q \)
- Drift velocity = \( v_d \)
In time \( t \), charge carriers move a distance:
\[
\ell = v_d t
\]
Step 2: Volume of Charge Flowing
Volume of conductor through which charges move:
\[
\text{Volume} = A \times \ell = A v_d t
\]
Number of charge carriers in this volume:
\[
N = n A v_d t
\]
Step 3: Total Charge Flow
Total charge crossing the section in time \( t \):
\[
Q = nqAv_d t
\]
Step 4: Relation with Electric Current
By definition of current:
\[
I = \frac{Q}{t}
\]
Substituting \( Q \):
\[
I = \frac{nqAv_d t}{t}
\]
\[
\boxed{I = nqAv_d}
\]
This is the required relation between current and drift velocity.
Special Case: Electrons as Charge Carriers
If electrons are charge carriers:
\[
q = e
\]
\[
I = neAv_d
\]
Direction:
- Electron drift is opposite to electric field
- Current direction is opposite to electron motion
Drift Velocity in terms of Electric Field
From microscopic theory:
\[
v_d = \mu E
\]
where \( \mu \) is mobility.
Thus:
\[
I = nqA\mu E
\]
This leads to Ohm’s law at microscopic level.
Key Observations:
- Current depends on number density of charge carriers.
- Larger cross-section gives larger current.
- Drift velocity is very small compared to speed of light.