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Flashcards · AP® Physics 2: Algebra-Based · Unit 11
Unit 11: Electric Circuits flashcards
53 cards on topics 11.1 to 11.8. Pick a topic or study the whole unit.
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11.1 Electric Current
- What is electric current?
- The rate at which charge passes through a cross-section of a conductor: I = ΔQ/Δt, in amperes (1 A = 1 C/s). It is measured at a place, not stored in a component.
- What is the direction of conventional current?
- The direction positive charge would move: from + to − outside the source. In metals, electrons carry the current and drift the opposite way.
- What is emf?
- The potential difference a source provides, ℰ, in volts. It is energy per unit charge, not a force. The source supplies energy; the charge carriers are already in the wire.
- How do you find the charge that passes when the current changes?
- Find the area under the I–t graph (A × s = C). Peak current × time overestimates it.
- About how many electrons carry 1.0 C of charge?
- N = ΔQ/e = 1.0 / (1.60 × 10⁻¹⁹) ≈ 6.25 × 10¹⁸ electrons.
- How do electrons move in a wire carrying a current?
- They already move randomly at about 10⁶ m/s with zero net motion. A potential difference adds a slow drift in one direction, and only the drift carries net charge.
- Is current used up in a component?
- No. The same current enters and leaves a component; energy is transferred, not charge.
11.2 Simple Circuits
- What is a closed circuit, an open circuit and a short circuit?
- Closed: a complete loop with a source, so charges can flow. Open: a break anywhere, so no current anywhere in that loop. Short: a path with no change in potential across an element, which then carries no current.
- How are ideal ammeters and voltmeters connected?
- An ammeter goes in the loop, so the current passes through it, and acts like a plain wire. A voltmeter goes across an element, one lead on each end, and lets no charge through.
- A plain wire is connected across one of two bulbs in a single loop. What happens to that bulb?
- It goes out. It is short-circuited: there is no potential difference across it, so no current through it.
- A battery is connected to two bulbs, each in its own branch. How many closed loops are there?
- Three: the battery with each bulb, and the loop through the two bulbs alone. Count loops without the battery too.
- Does wire length or position on a schematic matter?
- No. Schematics show connections only, and ideal wires have no change in potential along them. Crossing wires without a dot are not connected.
- What happens when a switch in a single loop is opened?
- There is no current anywhere in that loop, not just after the gap. Every element in the loop goes off.
11.3 Resistance, Resistivity, and Ohm’s Law
- What is resistance, and how is it defined?
- How strongly an object opposes the movement of charge: R = ΔV/I, in ohms (1 Ω = 1 V/A).
- What is the difference between resistance and resistivity?
- Resistivity ρ (Ω·m) is a property of the material. Resistance R = ρL/A is a property of one object and also depends on its length and cross-sectional area.
- A wire is replaced by one of the same metal with three times the length and twice the diameter. How does R change?
- Length × 3 gives R × 3. Diameter × 2 gives area × 4, so R ÷ 4. Overall R × 3/4.
- What does the slope of an I against ΔV graph tell you?
- Slope = 1/R, so a steeper line means a smaller resistance. A slope of 0.050 A/V gives R = 20 Ω.
- What is an ohmic element?
- One whose resistance is the same at every current, so I ∝ ΔV: its I–ΔV graph is a straight line through the origin. A curved graph through the origin is not ohmic.
- Why does a filament bulb's resistance rise as it glows?
- Its temperature rises, and the resistivity of most conductors increases with temperature: hotter atoms vibrate more and obstruct drifting electrons more often.
- How do you find resistivity from lab data?
- Measure R for different lengths of the same wire and plot R against L. The slope is ρ/A, so ρ = slope × A, with A = π(d/2)² in m².
11.4 Electric Power
- What is electric power in a circuit element?
- P = IΔV, energy per charge times charge per second, in watts (1 W = 1 J/s). It applies to every element.
- When do you use P = I²R and when P = ΔV²/R?
- P = I²R when elements share the same current (one loop): larger R, more power. P = ΔV²/R when they share the same ΔV (each across the same battery): smaller R, more power.
- The potential difference across a resistor doubles. What happens to its power?
- It multiplies by 4, since P = ΔV²/R at constant R. Tripling ΔV gives 9 times the power.
- Two bulbs share one loop. Which is brighter?
- The one with the larger resistance. They carry the same current, so P = I²R is bigger for the larger R. Brightness increases with power.
- How much energy does a 60 W lamp transfer in 5.0 minutes?
- ΔE = PΔt = 60 × 300 = 1.8 × 10⁴ J. Convert minutes to seconds.
- Does a bulb's power rating apply in every circuit?
- No. A rating such as "6.0 V, 3.0 W" applies only at the stated potential difference. A 12 W bulb can be dimmer than a 3 W bulb in some circuits.
- How is energy balanced in a circuit with an ideal battery?
- Energy supplied per second by the battery (Iℰ) equals the energy dissipated per second by resistors and bulbs, plus any being stored in a capacitor.
11.5 Compound Direct Current (DC) Circuits
- How do you combine resistors in series and parallel?
- Series: R_eq = R₁ + R₂ + … Parallel: 1/R_eq = 1/R₁ + 1/R₂ + …, then invert at the end. n identical resistors in parallel give R/n.
- What is the equivalent resistance of 12 Ω and 6.0 Ω in parallel?
- 1/R_eq = 1/12 + 1/6.0 = 3/12, so R_eq = 4.0 Ω, less than either resistor.
- What is shared in series and in parallel?
- Series: the same current in each element (only one path). Parallel: the same potential difference across each branch (both ends on the same two points).
- What is the terminal voltage of a real battery?
- ΔV_terminal = ℰ − Ir, where r is the internal resistance. With one external resistance, I = ℰ/(R + r). The emf equals the terminal voltage only when there is no current.
- A third bulb is added in parallel with two bulbs across an ideal battery. Does the first bulb get dimmer?
- No. Its potential difference is still the emf, so its current and power are unchanged; the battery supplies more total current.
- Why does a real voltmeter read slightly low?
- It has very large but finite resistance. In parallel it lowers the resistance of that part of the circuit, so the potential difference there falls slightly.
- A cell of emf 1.5 V and internal resistance 0.20 Ω carries 0.50 A. What is its terminal voltage?
- ΔV = ℰ − Ir = 1.5 − 0.50 × 0.20 = 1.4 V.
11.6 Kirchhoff’s Loop Rule
- What is Kirchhoff's loop rule?
- The sum of potential differences round any closed loop is zero: ΣΔV = 0. Each point has one potential, so it is energy conservation for charges.
- What are the sign rules for a loop equation?
- Battery crossed − to +: +ℰ; + to −: −ℰ. Resistor crossed with the current: −IR; against it: +IR. Keep one direction round the loop.
- A 1.5 V ideal cell drives a current through two resistors in series. One has 0.90 V across it. What is across the other?
- 1.5 − 0.90 = 0.60 V, by the loop rule.
- Does the loop rule apply to loops with no battery?
- Yes, to every closed loop. A loop through two parallel branches shows that they have equal potential differences.
- In a single loop, what decides each resistor's share of the voltage?
- Its resistance, not its position. With the same current, ΔV = IR is largest across the largest resistance.
- How much electric potential energy does 3.0 C lose passing through a resistor with 4.0 V across it?
- ΔU = qΔV = 3.0 × 4.0 = 12 J, converted to thermal energy in the resistor.
11.7 Kirchhoff’s Junction Rule
- What is Kirchhoff's junction rule?
- The total current into a junction equals the total current out: ΣI_in = ΣI_out. It follows from conservation of charge.
- At a junction, 4.0 A enters along one wire and 2.5 A leaves along a second. What does the third wire carry?
- 1.5 A, leaving the junction, so that 4.0 A in = 2.5 + 1.5 A out.
- How does current split between parallel branches?
- Each branch has the same ΔV, so I = ΔV/R: more current through the smaller resistance. Split equally only for identical branches.
- An ideal 6.0 V battery is across 4.0 Ω and 12 Ω in parallel. What are the currents?
- 6.0/4.0 = 1.5 A and 6.0/12 = 0.50 A; the battery carries 1.5 + 0.50 = 2.0 A.
- Which conservation laws are behind Kirchhoff's two rules?
- The junction rule is conservation of charge. The loop rule is conservation of energy. Most branched circuits need both.
- What does a negative answer for a current mean?
- The current flows opposite to the arrow you drew. Keep the sign; your choice of arrow was arbitrary.
11.8 Resistor-Capacitor (RC) Circuits
- How do you combine capacitors in series and parallel?
- Parallel: C_eq = C₁ + C₂ + … Series: 1/C_eq = 1/C₁ + 1/C₂ + … These are the reverse of the resistor rules. 3.0 μF and 6.0 μF give 2.0 μF in series and 9.0 μF in parallel.
- What is shared by series capacitors?
- The same charge Q, because the isolated inner plates keep zero net charge. Their ΔV values add, so the smallest capacitor has the largest ΔV.
- How does an uncharged capacitor behave just after the switch closes and after a long time?
- Just after closing it acts like a wire (ΔV_C = 0) and its branch current is largest. After many time constants it acts like a break, with zero current.
- What is the time constant of an RC circuit?
- τ = RC, in seconds (Ω × F = s). 10 kΩ and 100 μF give τ = 1.0 s. It depends only on R and C, not on the emf.
- How do current and charge change while a capacitor charges through a resistor?
- The current starts at ℰ/R and falls towards zero; Q, ΔV_C and stored energy rise towards their final values. Changes are fast at first, then slower.
- Roughly how charged is a capacitor after one time constant?
- About 63% of its final value, not full. Charging from 12 V, ΔV_C is about 7.6 V after one τ.
- What happens when a charged capacitor discharges through a resistor?
- Q, ΔV_C, current and stored energy all fall towards zero, fast at first then slower. The current in the capacitor's branch is reversed compared with charging.
Study Unit 11 further
- 11.1 Electric Current Study guide: 11.1 Electric CurrentRevision notes: 11.1 Electric CurrentPractice questions: 11.1 Electric Current
- 11.2 Simple Circuits Study guide: 11.2 Simple CircuitsRevision notes: 11.2 Simple CircuitsPractice questions: 11.2 Simple Circuits
- 11.3 Resistance, Resistivity, and Ohm’s Law Study guide: 11.3 Resistance, Resistivity, and Ohm’s LawRevision notes: 11.3 Resistance, Resistivity, and Ohm’s LawPractice questions: 11.3 Resistance, Resistivity, and Ohm’s Law
- 11.4 Electric Power Study guide: 11.4 Electric PowerRevision notes: 11.4 Electric PowerPractice questions: 11.4 Electric Power
- 11.5 Compound Direct Current (DC) Circuits Study guide: 11.5 Compound Direct Current (DC) CircuitsRevision notes: 11.5 Compound Direct Current (DC) CircuitsPractice questions: 11.5 Compound Direct Current (DC) Circuits
- 11.6 Kirchhoff’s Loop Rule Study guide: 11.6 Kirchhoff’s Loop RuleRevision notes: 11.6 Kirchhoff’s Loop RulePractice questions: 11.6 Kirchhoff’s Loop Rule
- 11.7 Kirchhoff’s Junction Rule Study guide: 11.7 Kirchhoff’s Junction RuleRevision notes: 11.7 Kirchhoff’s Junction RulePractice questions: 11.7 Kirchhoff’s Junction Rule
- 11.8 Resistor-Capacitor (RC) Circuits Study guide: 11.8 Resistor-Capacitor (RC) CircuitsRevision notes: 11.8 Resistor-Capacitor (RC) CircuitsPractice questions: 11.8 Resistor-Capacitor (RC) Circuits
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