Rate of flow of electric charge through a cross-section.
$$ I = \frac{dq}{dt} $$Unit: Ampere (A). It's a scalar quantity!
Average velocity of free electrons in a conductor under external electric field.
$$ v_d = -\frac{eE}{m}\tau $$$\tau = $ Relaxation time (time between collisions).
Current is directly proportional to potential difference (at constant temp).
$$ V = IR $$
Fails for non-ohmic devices (diodes, transistors, GaAs).
Depends on material & temperature, NOT geometry.
Metals: $\rho$ increases with T.
Semiconductors: $\rho$ decreases with T.
Series: Use $I^2R$ (higher R glows brighter).
Parallel: Use $V^2/R$ (lower R glows brighter).
Color Coding Mnemonic:
B B R O Y Great Britain Very Good Wife
Current is same across all.
Voltage is same across all.
EMF ($\varepsilon$): Potential difference when no current is drawn.
Terminal Voltage ($V$): Potential diff when current $I$ is drawn.
$$ V = \varepsilon - Ir $$
Sum of currents entering = Sum leaving. (Conservation of Charge)
Algebraic sum of changes in potential around closed loop is zero. (Conservation of Energy)
Assign a reference node (0V), name unknown nodes ($x$), and apply KCL:
$$ \sum I_{leaving} = 0 $$
Faster than KVL for complex circuits!
Balanced Condition ($I_g = 0$):
$$ \frac{R_1}{R_2} = \frac{R_3}{R_4} $$
Used to measure unknown resistance accurately.
Practical application of Wheatstone bridge. Null point at length $l$ cm:
$$ S = R \left( \frac{100 - l}{l} \right) $$
Connect low resistance (Shunt $S$) in parallel.
$$ S = \left( \frac{I_g}{I - I_g} \right) G $$Connect high resistance ($R$) in series.
$$ R = \frac{V}{I_g} - G $$