Electric Current & DC Circuit Summary
Attention-Grabbers & Context
- “ELECTRIFYING!!!, SHOCKING BUT TRUE!!!!, You will be ex-static!” – motivational phrases used to introduce the topic and signal excitement in Physics 11 (Mr. Stephenson, 2019).
- Focus: Direct-current (DC) electricity, its physical basis, and quantitative laws used for circuit analysis.
Fundamental Law of Electric Charges
- Key postulates:
- Opposite charges attract; like charges repel.
- Charged objects may attract neutral objects (polarization effects).
- Elementary charges:
- Electron charge: q_e=-1.6\times10^{-19}\,\text{C}
- Proton charge: q_p=+1.6\times10^{-19}\,\text{C}
- Neutron: q_n = 0
- All matter comprises protons, neutrons, electrons.
- Coulomb (C) = unit of electric charge.
Voltage (Electric Potential Difference)
- A battery’s internal chemical reaction separates charge, creating positive & negative terminals.
- Definition: Voltage (V) = electric potential energy per unit charge.
- V = \dfrac{E_{\text{potential}}}{Q}
- Unit: volt (V); 1\,\text{V}=1\,\text{J}/\text{C}
- Provides electrons in the external circuit with electric potential energy that can be converted to other forms by loads.
Electric Current
- Two conventions:
- Conventional current: flow of positive charge from + to –.
- Electron flow (the physical reality): electrons move from – to +.
- Definition: I = \dfrac{Q}{t}
- Unit: ampere (A); 1\,\text{A}=1\,\text{C}/\text{s}
- Charge–electron conversion example:
- Number of electrons in -1\,\text{C}:
\dfrac{-1\,\text{C}}{-1.6\times10^{-19}\,\text{C/e¯}} \approx 6.2\times10^{18}\,\text{electrons}
Resistance (R)
- Opposes the flow of electric charge; arises from collisions between charge carriers and lattice atoms.
- Consequences: charges lose electric potential energy → thermal energy, light, etc.
- Unit: ohm (Ω).
- Physical examples: light-bulb filament, stove heating element; commercial resistors with color-code bands.
Ohm’s Law
- Relationship between voltage, current, resistance:
- V = IR
- Linear for ohmic materials; slope in an I–V graph equals resistance.
Worked Examples (Ohm’s Law)
- Light bulb, R=20\,\Omega,\;V=5.0\,\text{V}:
- I = \dfrac{V}{R} = \dfrac{5.0}{20}=0.25\,\text{A}
- Motor, R=75\,\Omega,\;V=12\,\text{V}:
- I = \dfrac{12}{75}=0.16\,\text{A}
- Unknown battery voltage, I=0.80\,\text{A},\;R=25\,\Omega:
- V = IR =0.80\times25 = 20\,\text{V}
Standard Circuit Symbols (Table 3.1 excerpts)
- Cell: long line = +, short line = – ; represents a source of electric potential.
- Battery: several cells in series.
- Conducting wire: straight line.
- Load/Resistor: zig-zag line (R, Ω).
- Switch (open/closed): break or continuous line with pivot.
- Voltmeter: circle with V (measures V).
- Ammeter: circle with A (measures I).
Types of Circuits
Series Circuits
- Single path for current.
- Laws:
- Current: IS = I1 = I2 = I3 (same everywhere).
- Voltage: VS = V1 + V2 + V3.
- Equivalent resistance: RT = R1+R2+R3.
- Overall: IS = \dfrac{VS}{R_T}.
Parallel Circuits
- Two or more independent paths; current splits at junctions.
- Laws:
- Voltage: VS = V1 = V2 = V3 (same across each branch).
- Current: IS = I1 + I2 + I3.
- Equivalent resistance: \dfrac{1}{RP}=\dfrac{1}{R1}+\dfrac{1}{R2}+\dfrac{1}{R3}.
- Overall: IS = \dfrac{VS}{R_P}.
Combination (Series–Parallel)
- Real-world circuits often mix both configurations; analyze by reducing step-wise to a single equivalent resistance.
Kirchhoff’s Laws (Advanced Circuit Analysis)
- Kirchhoff’s Current Law (KCL):
- At any junction, \sum I{\text{in}} = \sum I{\text{out}}.
- Kirchhoff’s Voltage Law (KVL):
- For any closed loop, \sum (\Delta V) = 0 (sum of rises and drops is zero).
- Together with Ohm’s law and series/parallel R rules, allow complete solution of complex circuits.
Effects of Adding Loads & Safety Considerations
- Adding resistors in parallel ↓ R_T → ↑ total current.
- Excessive current risks:
- Device damage, wire overheating, fire.
- Mitigation: fuses & circuit breakers (open the circuit if current exceeds a preset threshold).
- Short circuit = unintended low-resistance path → very high I, causing shock & burns.
Electric Power
- Definition: P = \dfrac{E}{t}.
- Unit: watt (W); 1\,\text{W}=1\,\text{J/s}.
- Electrical expressions:
- Basic: P = VI.
- Substitutions via Ohm’s Law:
- P = I^2 R (replace V).
- P = \dfrac{V^2}{R} (replace I).
- Dimensional check: (J/C)\times(C/s)=J/s=W.
Power Examples
- 9 V battery, I=0.20\,\text{A}:
- P = VI = 9\times0.20 = 1.8\,\text{W}.
- Wire loss, I=50\,\text{A},\;R=0.10\,\Omega:
- P = I^2R=(50)^2\times0.10 = 250\,\text{W}.
Electric Energy & Billing
- Kilowatt-hour (kWh): energy used when P=1\,\text{kW} for 1\,\text{h}.
- 1\,\text{kWh} = 1000\,\text{W}\times3600\,\text{s}=3.6\times10^{6}\,\text{J}.
- Energy calculation: E = P t (convert units as needed).
- Example: Hair-dryer P=1200\,\text{W}=1.2\,\text{kW}, run 20 min = \tfrac{1}{3}\,\text{h}.
- E = 1.2\,\text{kW}\times\tfrac{1}{3}\,\text{h}=0.40\,\text{kWh}.
- Cost at 0.25\,\$/\text{kWh}: 0.40\times0.25=\$0.10.
Electromotive Force (emf), Internal Resistance & Terminal Voltage
- emf (symbol \varepsilon or \xi): open-circuit voltage of a source (no current drawn).
- Real sources possess internal resistance r.
- When current I flows, internal drop I r lowers terminal voltage V_{ab}:
- V_{ab}=\varepsilon - I r.
- Diagram conventions: positive terminal at higher potential; internal r in series with ideal emf source.
emf Example (Page 22)
- Given battery \varepsilon = 12.0\,\text{V}, internal r=0.50\,\Omega, external load R_L = 10.0\,\Omega (labeled 10.5 Ω total when including r):
- Total resistance: R{\text{tot}}=RL + r = 10.0 + 0.50 = 10.5\,\Omega.
- Current: I = \dfrac{\varepsilon}{R_{\text{tot}}} = \dfrac{12.0}{10.5}=1.14\,\text{A}.
- Terminal voltage: V_{ab}=\varepsilon - I r = 12.0 - (1.14)(0.50)=11.4\,\text{V}.
Practical & Ethical Considerations
- Understanding circuit behavior is critical to safe household wiring, appliance design, and prevention of electrical hazards.
- Engineers must weigh efficiency (minimizing I^2 R losses) against safety and cost.
- Awareness of internal resistance helps in battery selection for sensitive electronics.
Quick Reference: Key Equations
- I = \dfrac{Q}{t} V = IR RT^{\text{series}} = \sum Ri \dfrac{1}{RP}=\sum \dfrac{1}{Ri}
- P = VI = I^2 R = \dfrac{V^2}{R} E = P t V_{ab}=\varepsilon - I r