Resources | Subject Notes | Physics
This section covers the construction and analysis of series and parallel circuits. Understanding these circuit configurations is fundamental to electricity and electronics.
In a series circuit, components are connected end-to-end, forming a single path for the current. The current is the same through all components in a series circuit.
For a series circuit:
Component | Resistance (Ω) | Voltage Drop (V) | Current (A) |
---|---|---|---|
Resistor 1 | $R_1$ | $V_1$ | $I$ |
Resistor 2 | $R_2$ | $V_2$ | $I$ |
Resistor 3 | $R_3$ | $V_3$ | $I$ |
In a parallel circuit, components are connected across each other, providing multiple paths for the current. The voltage is the same across all components in a parallel circuit.
For a parallel circuit:
Component | Resistance (Ω) | Voltage (V) | Current (A) |
---|---|---|---|
Resistor 1 | $R_1$ | $V$ | $I_1$ |
Resistor 2 | $R_2$ | $V$ | $I_2$ |
Resistor 3 | $R_3$ | $V$ | $I_3$ |
Understanding how to calculate the total resistance and total current in series and parallel circuits is crucial. These calculations involve applying the appropriate formulas based on the circuit configuration.
The total resistance in a series circuit is simply the sum of the individual resistances.
$R_{total} = R_1 + R_2 + R_3 + ...$
The reciprocal of the total resistance in a parallel circuit is the sum of the reciprocals of the individual resistances.
$\frac{1}{R_{total}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + ...$
The total current in a parallel circuit is the sum of the currents flowing through each branch.
$I_{total} = I_1 + I_2 + I_3 + ...$
Series and parallel circuits are used in a wide variety of applications, including: