Chapter 4 - Electric Circuits
Current
- Current: the amount of charge passing a point in a given time period
- ==I = ΔQ/Δt==
- I: current (Amperes)
- Q: charge (Coulombs)
- t: time (seconds)
- Current is described in the AP exam as the flow of positive charge
Ohm’s Law
- Batteries: create currents using a difference in potential
- The “+” terminal has a higher electric potential
- The “-” terminal has a lower electric potential
- Generally, the greater the potential difference, the more current flows
- Resistance: a property of the circuit that resists the current
- Units are Ohms (Ω)
- ==R = ⍴L/A==
- R: resistance
- ⍴: resistivity
- L: length of wire
- A: cross-sectional area of wire
- Ohm’s Law
- ==I = ΔV/R==
- ΔV: voltage across a certain part of the circuit (like a resistor)
- R: resistance
- I: current
- Power: the rate at which electrical energy is converted to heat energy
- ==P = IΔV = I^2 R = ΔV^2/R==
- Ohmic vs. Nonohmic
- Ohmic: a circuit part (resistor or capacitor) that maintains the same resistance when the voltage across it or current through it changes - resistance is constant
- Circuit Pictures
- Wire: straight line
- Battery: 4 parallel lines - one long line and then one smaller line repeated
- Resistor: zig zag line
- Capacitor: 2 parallel lines
- Resistors in Series
- ==R = ⅀Ri==
- Ri: the resistances of the resistors in series with each other
- R: equivalent resistance or total resistance
- Resistors in Parallel
- ==1/R = ⅀1/Ri==
- Ri: the resistances of the resistors in parallel with each other
- R: equivalent resistance or total resistance
- Rules for resistors in circuits
- The current in resistors in series is equal to each other
- The voltage across resistors in parallel is equal to each other
- The voltage across two resistors in parallel is also equal to the voltage across each individual resistor
- V-I-R charts
- Create columns of V, I, and R for each individual resistor and the total circuit
- This helps us stay organized in complex problems
Kirchhoff’s Rules
- Junction Rule: The current entering and leaving a junction is equal
- Loop Rule: In a closed loop, the sum of the voltages is 0
- Choose a loop of the circuit and when you see a resistor, the voltage is -IR because resistors resist the current
- If the loop is against the current, the voltage is +IR
- When you see a batter, add the voltage of the battery (if going from - to +)
- If you go from + to -, subtract the voltage of the battery
- If the current you calculate is negative, you chose the wrong direction and the current flows the opposite way
Experimental Circuits
- In calculations, we assume most electronic devices in circuits act as resistors
- Light bulb
- The brightness of a bulb depends only on the power dissipated
- The power of a bulb can change depending on the current and voltage of the circuit it’s in
- Ammeters and Voltmeters
- Ammeters: measure current
- Ammeters work by putting them in series with resistors (current is constant for resistors in series)
- Voltmeters: measure potential difference (voltage)
- Voltmeters work by putting them parallel to parallel resistors
- Real batteries
- In a perfect world, batteries have no resistance but in the real world, this is not true
- The voltage advertised by a battery, ε, is actually larger than the real voltage ΔV (terminal voltage)
- ==ΔV = ε - Ir==
- r: the internal resistance of the battery
- I: current through the battery
- Internal resistance is measured by hooking a battery up to a resistor and plotting the terminal voltage of the battery as a function of the current through the battery
- The slope will be equal to -r
- Switches
- Open switch: that part (loop) of the circuit can be considered gone (dead)
- Capacitors
- Capacitors: two parallel metal plates separated by either air or dielectric material
- Capacitance: how much charge a capacitor can hold for each volt of potential difference
- ==C = kεA/d==
- C: capacitance
- k: dielectric constant
- ε: vacuum permittivity constant
- A: area of one of the plates (both plates have the same area)
- d: distance between plates
- ==ΔV = Q/C==
- ΔV: Voltage
- Q: charge
- C: capacitance (Farads)
- ==U = 1/2 QΔV = 1/2 C(ΔV )^2==
- U: energy stored in a capacitor
- Q: charge
- ΔV: potential difference
- C: capacitance
- ==ΔV/Δr = E==
- E: electric field
- ΔV: potential difference
- Δr: distance between plates
- Parallel vs. Series Capacitors
- Parallel Capacitors
- ==C = ⅀Ci==
- C: total capacitance for capacitors in parallel
- Ci: capacitance of capacitors in parallel
- This is the same formula from resistors in series - capacitors are basically resistors in reverse
- Series Capacitors
- ==1/C = ⅀1/Ci==
- C: total capacitance for capacitors in series
- Ci: capacitance of capacitors in series
RC Circuits
- RC Circuit: a circuit containing resistor(s) and capacitor(s)
- You’ll only be asked about RC Circuits in certain states
- When you first connect a capacitor to a circuit:
- No charge has built up so treat the capacitor like a wire with no potential difference
- After a long time:
- The capacitor has charged up to its max so no current will flow through it
- Treat the capacitor like an open switch
- The potential difference across the capacitor equals the voltage of the devices parallel to the capacitor