Electronic Components
- Basic Electronics - Hall Effect
- Basic Electronics - Semiconductors
- Basic Electronics - Energy Bands
- Basic Electronics - Materials
Resistors
- Basic Electronics - Fixed Resistors
- Basic Electronics - Linear Resistors
- Non-linear Resistors
- Circuit Connections in Resistors
- Basic Electronics - Resistors
Capacitors
- Polarized Capacitors
- Basic Electronics - Fixed Capacitors
- Variable Capacitors
- Circuit Connections in Capacitors
- Basic Electronics - Capacitors
Inductors
- Basic Electronics - RF Inductors
- Types of Inductors
- Circuit Connections in Inductors
- Basic Electronics - Inductance
- Basic Electronics - Inductors
Transformers
- Transformer Efficiency
- Transformers based on Usage
- Types of Transformers
- Basic Electronics - Transformers
Diodes
- Optoelectronic Diodes
- Special Purpose Diodes
- Basic Electronics - Junction Diodes
- Basic Electronics - Diodes
Transistors
- Basic Electronics - MOSFET
- Basic Electronics - JFET
- Types of Transistors
- Transistor Load Line Analysis
- Transistor Regions of Operation
- Transistor Configurations
- Basic Electronics - Transistors
Basic Electronics Useful Resources
Selected Reading
- Who is Who
- Computer Glossary
- HR Interview Questions
- Effective Resume Writing
- Questions and Answers
- UPSC IAS Exams Notes
Circuit Connections in Capacitors
In a circuit, a Capacitor can be connected in series or in parallel fashion. If a set of capacitors were connected in a circuit, the type of capacitor connection deals with the voltage and current values in that network.
Capacitors in Series
Let us observe what happens, when few Capacitors are connected in Series. Let us consider three capacitors with different values, as shown in the figure below.
Capacitance
When the capacitance of a network whose capacitors are in series is considered, the reciprocal of the capacitances of all capacitors, is added to get the reciprocal of the total capacitance. To get this more clearly,
$$frac{1}{C_{T}}::=::frac{1}{C_{1}}::+::frac{1}{C_{2}}::+::frac{1}{C_{3}}$$
Following the same formula, if simply two capacitors are connected in series, then
$$C_{T}::=::frac{C_{1}:: imes::C_{2}}{C_{1}::+::C_{2}}$$
Where C1 is the capacitance across the 1st capacitor, C2 is the capacitance across the 2nd capacitor and C3 is the capacitance across the 3rd capacitor in the above network.
Voltage
The voltage across each capacitor depends upon the value of inspanidual capacitances. Which means
$$V_{C1}::=::frac{Q_{T}}{C_{1}}::V_{C2}::=::frac{Q_{T}}{C_{2}}::V_{C3}::=::frac{Q_{T}}{C_{3}}$$
The total voltage across the series capacitors circuit,
$$V_{T}::=::V_{C1}::+::V_{C2}::+::V_{C3}$$
Where Vc1 is the voltage across the 1st capacitor, Vc2 is the voltage across the 2nd capacitor and Vc3 is the voltage across the 3rd capacitor in the above network.
Current
The total amount of Current that flows through a set of Capacitors connected in series is the same at all the points. Therefore the capacitors will store the same amount of charge regardless of their capacitance value.
Current through the network,
$$I::=::I_{1}::=::I_{2}::=::I_{3}$$
Where I1 is the current through the 1st capacitor, I2 is the current through the 2nd capacitor and I3 is the current through the 3rd capacitor in the above network.
As the current is same, the storage of charge is same because any plate of a capacitor gets its charge from the adjacent capacitor and hence capacitors in series will have the same charge.
$$Q_{T}::=::Q_{1}::=::Q_{2}::=::Q_{3}$$
Capacitors in Parallel
Let us observe what happens, when few capacitors are connected in Parallel. Let us consider three capacitors with different values, as shown in the figure below.
Capacitance
The total Capacitance of the circuit is the equivalent to the sum of the inspanidual capacitances of the capacitors in the network.
$$C_{T}::=::C_{1}::+::C_{2}::+::C_{3}$$
Where C1 is the capacitance across the 1st capacitor, C2 is the capacitance across the 2nd capacitor and C3 is the capacitance across the 3rd capacitor in the above network.
Voltage
The voltage measured at the end of the circuit is same as the voltage across all the capacitors that are connected in a parallel circuit.
$$V_{T}::=::V_{1}::=::V_{2}::=::V_{3}$$
Where Vc1 is the voltage across the 1st capacitor, Vc2 is the voltage across the 2nd capacitor and Vc3 is the voltage across the 3rd capacitor in the above network.
Current
The total current flowing is equal to the sum of the currents flowing through each capacitor connected in the parallel network.
$$I_{T}::=::I_{1}::+::I_{2}::+::I_{3}$$
Where I1 is the current through the 1st capacitor, I2 is the current through the 2nd capacitor and I3 is the current through the 3rd capacitor in the above network.
Advertisements