CHPTR 26 Notes: Kirchoff's Rules & RC Circuits
Kirchhoff’s Rules
Application of Kirchhoff’s Rules:
Analyzing complex circuits is simplified by the use of Kirchhoff’s rules.
Current (or Junction) Rule:
Definition: The sum of the currents entering/leaving any junction point is zero.
Mathematical Representation: In the example at junction ‘a’:
I1 + I2 - I_3 = 0Implication: Indicates conservation of charge at any junction.
Voltage (or Loop) Rule:
Definition: The sum of potential differences across all elements around any closed loop is zero.
Mathematical Representation:
ext{Sum of } igtriangleup V = 0Implication: Indicates energy conservation in closed circuits.
Voltage Across Elements
Voltage Change Representation:
The voltage changes across each element as it is traversed from left to right is shown.
Important for applying Kirchhoff’s Voltage Rule in practical scenarios.
Solving Circuit Problems
Equation Requirement:
To solve a circuit problem, the number of independent equations needed equals the number of unknown quantities.
RC Circuits
Definition of RC Circuit:
A circuit consisting of a resistor (R) and a capacitor (C) connected in series.
Purpose: To control how quickly electric current increases or decreases within the circuit.
Key Characteristic: Do not deal with a constant value of electric current.
Applications of RC Circuits:
Commonly utilized as “high-pass” and “low-pass” filters for specific frequencies.
Other applications include:
Blinking lights
Turn signals
Windshield wipers
Pacemakers
Strobe lights
Flashbulbs
“ON/OFF” processes
Kirchhoff’s Application in RC Circuits:
When Kirchhoff’s rule is applied to a resistor and capacitor in series with a voltage source, the following is derived:
The product of R and C is referred to as the “time constant” (denoted as $ au$) of the circuit.
Mathematical Formulation:
RC = au
rac{dq}{dt} + rac{q}{RC} = - rac{ ext{ε}}{RC}
Where $ ext{ε}$ is the electromotive force (emf) applied to the circuit.
Distinct Stages in RC Circuits:
There are two key phases:
Charging the Capacitor:
Involves the rate of charge into the capacitor.
Discharging the Capacitor:
Involves the rate of charge leaving the capacitor.
Charging Capacitors through a Resistor
Charge Function Over Time:
Formula applying to the charge on the capacitor as a function of time:
Q(t) = C ext{ε}(1 - e^{-t/RC})Current During Charging:
Current can be expressed as:
i(t) = rac{ε}{R} e^{-t/RC}Where $Q$ is the charge at any given time $t$ and $C$ is the capacitance.
Discharging a Capacitor
Discharge Dynamics:
As the capacitor discharges through the resistor, the equation governing the circuit is:
R rac{di}{dt} + rac{q}{C} = 0
Current and Voltage for Discharging Capacitor:
The equations representing the current and voltage during a discharging phase are:
Current:
i(t) = - rac{Q}{RC} e^{-t/RC}Voltage:
V(t) = Q imes rac{1}{C} e^{-t/RC}