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AP Physics 2
Everything you need to plan, present and check understanding for AP Physics 2.
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Scoring rubrics
Point-by-point rubrics for all 134 free-response problems, with a score sheet. Free with the Physics list.
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Course outline
Official units, learning objectives and where each is taught.
Teaching guide
Lesson rhythm, exam format and unit-by-unit notes.
Student learning path
What students see: topic chapters, readings and checks.
Units, topics and misconceptions
Open a unit to see its topics, the learning objectives each one covers, the misconceptions students commonly bring and notes for teaching it.
Unit 9Thermodynamics
Build from this unit Practice set Solutions
Topic chapters: Thermal physics and gases
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9.1 Kinetic Theory of Temperature and Pressure
Common misconceptions
- “At thermal equilibrium all atoms move at the same speed.” A distribution of speeds remains. Equal temperature means equal average translational kinetic energy, not identical atom speeds.
- “A heavier gas must be hotter if it has more total kinetic energy.” Temperature tracks average energy per atom. Total energy also depends on how many atoms there are.
- “Pressure only exists where gas hits a real wall.” A small imagined surface anywhere in a gas experiences momentum exchange from atoms on both sides; pressure is a local property.
Teaching notes
- Work through the two-atom component-table example before assigning q01. Ask students to write two separate momentum equations and then perform the total kinetic-energy check; momentum conservation alone does not establish an elastic collision.
- Ask students to draw incoming and outgoing velocity components before calculating an impulse. The normal component reverses at an ideal smooth wall; the tangential component does not.
- For two gases at the same temperature ask separately about average kinetic energy, rms speed, and total internal energy. These are different questions.
- Use qualitative distribution sketches. Do not require the functional formula of the Maxwell–Boltzmann distribution or three-dimensional collision calculations.
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9.2 The Ideal Gas Law
Common misconceptions
- “If the temperature doubles in degrees Celsius, pressure doubles.” Gas-law ratios require kelvin. For example, 20 °C to 40 °C changes 293 K to 313 K, a much smaller ratio.
- “PV is always constant.” PV is constant only when both amount and temperature are fixed.
- “Extrapolating a gas graph proves a real gas remains gaseous to absolute zero.” Extrapolation describes the ideal model; real gases often liquefy before that limiting state.
Teaching notes
- Have students annotate fixed N, V, P, or T directly on each graph.
- Check use of absolute pressure if a device reports gauge pressure. Add ambient pressure before applying PV = nRT.
- Accept a zero-pressure intercept close to −273 °C from uncertain data, with an explanation of the ideal-model extrapolation.
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9.3 Thermal Energy Transfer and Equilibrium
Common misconceptions
- “An object contains heat.” An object has internal energy. Heat describes transfer across a boundary because of a temperature difference.
- “Equal temperatures mean no atom-level energy exchanges occur.” Collisions and radiation can still exchange energy in both directions; equilibrium means no net thermal transfer.
- “The larger or more energetic object always heats the smaller one.” The spontaneous net direction depends on temperature, not total energy or mass.
Teaching notes
- Use arrows crossing a drawn boundary. Ask whose Q is positive and whose is negative for the same interaction.
- Ask students to classify mechanism and direction separately: radiation can carry energy across empty space; direction follows temperature.
- At equilibrium press for the words no net transfer, rather than no transfer.
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9.4 The First Law of Thermodynamics
Common misconceptions
- “An isothermal expansion has Q = 0.” For an ideal gas ΔU = 0 when T is fixed, but expansion gives W_on < 0. Heating supplies Q = −W_on > 0.
- “Work is a property stored in a state.” Work is a transfer that depends on the path. Internal energy is a state property.
- “Compression always cools a gas.” Adiabatic compression adds energy by work and heats it. Cooling can occur if enough energy leaves thermally.
- “A closed system cannot exchange energy.” Closed means matter does not cross its boundary. Energy can cross by heat or work; an isolated system exchanges neither matter nor energy.
Teaching notes
- Require a signed energy ledger before substitution: Q into gas positive, W_on from compression positive.
- On each PV path, mark direction. The area alone gives a magnitude; expansion or compression gives the work sign.
- Keep U = 3nRT/2 explicitly limited to an ideal monatomic gas; it is not a formula for solids or arbitrary molecular gases.
- When using gas pressure for PV work, state slow mechanical equilibrium with the external pressure. For irreversible expansion use external pressure, not an unspecified gas pressure.
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9.5 Specific Heat and Thermal Conductivity
Common misconceptions
- “Specific heat and heat capacity are the same quantity.” Specific heat c is energy per kilogram per kelvin; the sample’s heat capacity mc also depends on its mass.
- “A material with high conductivity must have low specific heat.” Conductivity and specific heat describe different microscopic behavior. One governs transfer rate; the other energy required for a temperature change.
- “A thick insulator changes its material conductivity.” Its geometry changes transfer rate, but the material’s intrinsic k stays the same under the stated conditions.
Teaching notes
- For calorimetry, students should name the combined system and every omitted energy store before setting energy gained equal to energy lost.
- Use the AP approximation of temperature-independent c, and avoid unprovided phase changes in Q = mcΔT problems.
- A steady conduction experiment needs two maintained boundary temperatures. A warming sample’s transient temperature curve is not automatically a measurement of k.
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9.6 Entropy and the Second Law of Thermodynamics
Common misconceptions
- “Entropy is simply the everyday messiness of an object.” Use the distribution of energy and the system’s thermodynamic state. Visual untidiness by itself is not a reliable thermodynamic measure.
- “If entropy rises, some energy disappears.” Energy remains conserved. It becomes more dispersed and less available to produce organized work under the given conditions.
- “Entropy of every object must increase.” A closed object can lose entropy through its surroundings. The entropy of the isolated combined system cannot decrease.
- “Two paths to the same final state produce different changes in the object’s entropy.” The object’s entropy is a state function, so the same endpoints give the same change; total entropy generation can differ.
Teaching notes
- Ask students to draw a larger boundary including the surroundings when a subsystem’s entropy decreases.
- Qualitative arguments are the AP requirement. Do not require ΔS = Q_rev/T, logarithmic gas formulas, or statistical entropy calculations.
- Distinguish entropy change of a returning cyclic device from entropy change of the device plus reservoirs.
- Describe reversible as an ideal limit that can be undone leaving no net change in both system and surroundings; ordinary finite-temperature-difference heat transfer is irreversible.
Unit 10Electric Force, Field, and Potential
Build from this unit Practice set Solutions
Topic chapters: Charge and electric fields, Electric energy, potential, and capacitors
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10.1 Electric Charge and Electric Force
Common misconceptions
- “A larger charge feels the larger force in a two-object interaction.” Both forces have magnitude k|q₁q₂|/r²; differing accelerations can come from different masses.
- “Neutral material has no electric forces.” Neutral matter contains charged constituents; microscopic electric interactions also underlie contact forces.
Teaching notes
- Ask students to explain force direction without using a negative magnitude.
- Have students state the point-charge and medium assumptions before using Coulomb’s law.
- Diagnose scale reasoning with a neutral planet versus a charged dust grain.
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10.2 Conservation of Electric Charge and the Process of Charging
Common misconceptions
- “Rubbing creates negative charge.” Electrons transfer between objects; the combined system’s charge is conserved.
- “Any grounded object must become neutral immediately.” A nearby charged source can maintain an induced net charge while the object is at ground potential.
Teaching notes
- Have students draw a boundary for object-only and object-plus-Earth systems.
- Ask which step crosses that boundary and which merely changes distribution.
- Use identical spheres only when claiming equal final charge.
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10.3 Electric Fields
Common misconceptions
- “Electric field points in the direction an electron accelerates.” Field direction uses positive charge; an electron’s acceleration is opposite.
- “Field lines are charged-particle trajectories.” They show force direction at each place. A particle’s existing velocity can make its path differ.
Teaching notes
- Require separate source-field sketches before net vectors.
- Ask why a tangential surface field contradicts conductor equilibrium.
- Use qualitative reasoning only for fields within general insulators.
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10.4 Electric Potential Energy
Common misconceptions
- “Negative energy means negative force magnitude.” Energy is a signed scalar relative to a reference. A force magnitude is nonnegative, with direction treated separately.
Teaching notes
- Ask students to narrate the sign of external work before multiplying numbers.
- Have them list pair labels to expose double counting.
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10.5 Electric Potential
Common misconceptions
- “Potential is a vector because electric field is a vector.” Potential is signed energy per charge; add it as a scalar.
- “A charged conductor must have zero potential because its internal field is zero.” Zero internal field implies one constant potential; its value depends on the reference and configuration.
Teaching notes
- Have students make both scalar and vector predictions at a dipole midpoint.
- Ask for contour labels and normal distance before estimating E.
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10.6 Capacitors
Common misconceptions
- “A capacitor stores a net charge Q.” The ideal plates carry +Q and −Q; Q labels a plate-charge magnitude and the complete capacitor has zero net charge.
- “Adding a dielectric always decreases capacitor energy.” It decreases energy at fixed charge but increases it at fixed voltage; the battery participates in the latter energy transfer.
Teaching notes
- Require a constraint statement before factor-of-change predictions.
- Ask students to connect the triangular area of the V versus Q graph to work.
- Check that projectile calculations satisfy the stated gap and negligible-edge assumptions.
- Distinguish the area under capacitor voltage versus charge (stored energy/minimum quasistatic assembly work) from constant-voltage battery energy QV. In ordinary RC charging the remainder is resistor heating.
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10.7 Conservation of Electric Energy
Common misconceptions
- “Every charged particle speeds up toward lower potential.” Positive charges do; negative charges can gain kinetic energy toward higher potential.
- “Potential difference by itself sets speed.” Charge, mass, initial kinetic energy, and any other work also matter.
Teaching notes
- Ask students to draw energy bars and state whether external work is included.
- Use a turning-point question to expose negative-K arithmetic as a physical impossibility.
- Ask whether all velocity components vanish at the proposed turning point. Without one-dimensional motion, K₀/q gives an energy accessibility bound rather than a guaranteed turning-potential rise.
Unit 11Electric Circuits
Build from this unit Practice set Solutions
Topic chapters: Current, resistance, and circuits
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11.1 Electric Current
Common misconceptions
- “The battery sends newly created electrons through a bulb.” Mobile charges already occupy the conducting circuit; the source transfers energy and maintains a potential difference.
- “No current means no electron motion.” It means no net organized charge flow, while random motion remains.
Teaching notes
- Have students distinguish a charge-flow rate from carrier drift speed.
- Ask students to redraw electron arrows without changing the conventional-current schematic.
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11.2 Simple Circuits
Common misconceptions
- “An open circuit has no voltage anywhere.” It lacks a conducting path through the break, but sources and the open gap can have nonzero potential difference.
- “Any two components drawn side by side are parallel.” They must connect to the same two nodes.
Teaching notes
- Have students build one schematic then redraw it in two shapes.
- Use the symbol figure and require students to identify a variable-element arrow.
- Check the battery’s shared membership in both loops.
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11.3 Resistance, Resistivity, and Ohm’s Law
Common misconceptions
- “Every ohmic metal has temperature-independent resistivity.” Constant-R ohmic behavior is usually specified at a controlled temperature. Real metallic ρ can rise with temperature; the temperature-independent idealization must be named.
- “I-versus-V slope equals resistance.” It equals 1/R; a V-versus-I slope equals R.
Teaching notes
- Read both axes aloud before extracting R.
- Have students identify which assumptions make constant ρ legitimate.
- Use low-current readings and cooldowns in resistance measurements.
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11.4 Electric Power
Common misconceptions
- “Current is used up as light is produced.” Energy is transferred and converted; charge flow is conserved through an unbranched bulb path.
- “Battery voltage can be used in every resistor’s P = V²/R.” Only use the voltage across the element whose power you are finding.
Teaching notes
- Demand a fixed-current or fixed-voltage statement in brightness comparisons.
- Ask students to check battery supplied power against sum of resistor powers.
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11.5 Compound Direct Current (DC) Circuits
Common misconceptions
- “All parallel branches carry the same current.” They share voltage; branch current depends on each resistance.
- “Battery emf always equals terminal voltage.” A discharging nonideal battery loses Ir internally; emf is its open-circuit voltage.
- “A voltmeter belongs in the same series path as the resistor.” It connects across the resistor’s endpoints; an ideal series voltmeter would interrupt current.
Teaching notes
- Check endpoints before reduction.
- Have students recover branch values after finding equivalent resistance.
- Ask why neglecting wire resistance fails in a nearly shorted loop.
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11.6 Kirchhoff’s Loop Rule
Common misconceptions
- “Every resistor is a negative term in every loop equation.” It is negative when traversal follows current and positive when traversal goes against current.
- “Every drawable loop adds an independent equation.” Some loop equations follow from others; use independent loops to solve, additional loops to check.
Teaching notes
- Require students to point to a physical element for each algebraic term.
- Ask them to redraw their potential graph after changing only the reference.
- Use explicit branch currents rather than ambiguous I labels.
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11.7 Kirchhoff’s Junction Rule
Common misconceptions
- “The current divides equally at every junction.” Branch currents depend on resistances and shared voltage; equality needs symmetry.
- “A negative solved current means the circuit is impossible.” It generally means the actual direction opposes your assumed arrow.
Teaching notes
- Ask for a region boundary around the junction and charge amounts over one second.
- Require a final arrow redraw when a solution is negative.
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11.8 Resistor-Capacitor (RC) Circuits
Common misconceptions
- “An uncharged capacitor acts like a wire forever.” It has zero voltage only initially; its branch current decreases as voltage builds, approaching an open-circuit endpoint.
- “Charge crosses the insulating gap while the capacitor charges.” Charge reaches one plate and leaves the other through external wires; the ideal dielectric does not conduct across the gap.
- “Every capacitor in series has equal voltage.” The standard series string has equal charge magnitude; voltage is Q/C and can differ.
Teaching notes
- Require initial state before choosing a wire or open-circuit model.
- Ask whether other branches still conduct at the final time.
- Use qualitative transient curves and τ landmarks; avoid exponential/logarithmic assessment.
Unit 12Magnetism and Electromagnetism
Build from this unit Practice set Solutions
Topic chapters: Magnetism and induction
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12.1 Magnetic Fields
Common misconceptions
- “Magnetic field lines begin at north and end at south.” Only the outside part looks that way. Follow the line through the magnet: it is closed.
- “Any iron sample must already be a strong permanent magnet.” Domains can cancel at the sample scale. Composition enables ferromagnetism; domain arrangement determines the net magnetization.
- “Permeability is always one fixed material constant.” Use the value for the specified temperature, orientation, and field strength.
Teaching notes
- Have students draw a full loop, including the magnet interior, before using a compass.
- Ask students to explain why a uniformly magnetized sample can still have two poles after cutting.
- Separate compass torque from a net translational force.
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12.2 Magnetism and Moving Charges
Common misconceptions
- “A negative charge has a negative force magnitude or radius.” Use |q| in magnitudes and radius. Its sign reverses the force direction.
- “Magnetic force accelerates a particle by making it faster.” Acceleration can change direction only. A magnetic-only force does no work.
- “The magnetic field created by a charge points along the force on that charge.” The source field and force are different vectors governed by different right-hand-rule inputs.
Teaching notes
- Require a labeled v, B, and F diagram before calculations.
- Quantitative moving-charge force questions use 0°, 90°, and 180°; discuss other angles qualitatively.
- The magnetic model is nonrelativistic and must keep v below c.
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12.3 Magnetism and Current-Carrying Wires
Common misconceptions
- “The field of a straight wire points away from the wire.” It is tangent to a circle centered on the wire, with no radial component.
- “Add the field magnitudes of two wires before checking directions.” Determine each local vector first; opposite fields subtract.
- “Use the whole wire length in IℓB.” Only the portion inside the stated field belongs in ℓ.
Teaching notes
- Use a compass map and then replace compass needles with tangent arrows.
- Ask for a straight-line B versus 1/r graph with slope units.
- Require separate diagrams for a source’s own field and force from an external field.
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12.4 Electromagnetic Induction and Faraday’s Law
Common misconceptions
- “Lenz’s law always makes a field opposite the existing field.” It opposes the change. A decreasing field is supported by a field in the same direction.
- “The angle in BA cos θ is measured from the surface.” Measure from its perpendicular area vector.
- “A generator gets electrical energy directly from a static magnetic field.” An external agent supplies work against the induced resisting force.
Teaching notes
- Have students choose one normal and associated positive circulation before assigning algebraic signs.
- Distinguish an induced emf from a current; a closed path is needed for sustained current.
- Use piecewise linear flux graphs so AP algebra gives the interval emfs.
Unit 13Geometric Optics
Build from this unit Practice set Solutions
Topic chapters: Light rays and images
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13.1 Reflection
Common misconceptions
- “A ray lies along a wavefront.” A ray is perpendicular to a wavefront and points in the propagation direction.
- “Reflection angles are measured from the mirror surface.” The law uses the normal, perpendicular to the local surface.
- “Diffuse reflection breaks the reflection law.” Every local patch obeys the law; its normal differs from neighboring patches.
Teaching notes
- Draw arrows on incident and reflected rays; missing arrows can hide a reversed path.
- Use a mirror and matte paper to compare reflected directions at the same incident angle.
- Discuss laser ray models alongside a slit demonstration, while leaving interference calculations to Unit 14.
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13.2 Images Formed by Mirrors
Common misconceptions
- “A negative image distance is an impossible answer.” It identifies a virtual image behind the mirror in the chosen convention.
- “A mirror focus is at its center of curvature.” For near-axis rays it is approximately halfway there.
- “All virtual mirror images are reduced.” A concave mirror used inside its focal length gives an enlarged virtual image.
Teaching notes
- State the optical sign convention on the board and reuse it for every problem.
- Ask learners to point to actual ray intersections before calling an image real.
- Limit mirrors to plane, concave spherical, and convex spherical; use near-axis rays for spherical equations.
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13.3 Refraction
Common misconceptions
- “Light changes frequency when it enters glass.” A stationary boundary keeps the source frequency fixed; speed and wavelength change.
- “Any sufficiently steep incidence can cause total internal reflection.” The ray must first be going from higher index to lower index.
- “An inverse-sine input above one means round the angle to 90°.” It means no real transmitted ray exists under the stated conditions.
Teaching notes
- Have learners identify medium 1 from the incoming arrow, rather than from table order.
- Use a semicircular block so the incoming ray can enter normally at its curved surface; this isolates refraction at the flat face.
- Check the two TIR conditions in words before calculating a critical angle.
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13.4 Images Formed by Lenses
Common misconceptions
- “A convex lens always forms a real image.” A real object inside its focal length gives an upright enlarged virtual image.
- “Both lens focal points are used the same way for every ray.” For a converging lens, parallel incident rays head through the far focus; near-focus incident rays exit parallel.
- “The image is negative because it is left on the drawing.” Optical signs distinguish real and virtual; the drawing can be reversed without changing those signs.
Teaching notes
- Begin with a labeled object, lens midline, both foci, and travel direction.
- Pair a screen projection outside f with direct viewing through the lens inside f.
- The rays model supports thin-lens and Snell/TIR cases; use static sketches for mirrors and diverging-lens details.
Unit 14Waves, Sound, and Physical Optics
Build from this unit Practice set Solutions
Topic chapters: Waves and sound, Light as a wave
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14.1 Properties of Wave Pulses and Waves
Common misconceptions
- “The crest is a piece of matter traveling down the rope.” A crest is a moving pattern. Follow a mark on the rope to see local oscillation while the disturbance and energy travel.
Teaching notes
- Mark one rope segment and ask whether it reaches the far end. Ask students to identify compression from a pressure graph rather than from a drawing of particles.
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14.2 Periodic Waves
Common misconceptions
- “The distance between two crests on any graph is wavelength.” Check the horizontal units: crest separation in seconds is period; separation in meters is wavelength.
Teaching notes
- Show identical-looking curves with x and t axes and ask which gives wavelength. Ask what is being held fixed before an energy comparison.
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14.3 Boundary Behavior of Waves and Polarization
Common misconceptions
- “An inverted reflected wave has negative frequency.” Inversion is a π phase reversal of signed displacement; frequency remains the positive repetition rate.
Teaching notes
- Use two strings at the same tension to establish the speed/phase rule. Do not generalize that rule to arbitrary impedance systems without specifying the model.
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14.4 Electromagnetic Waves
Common misconceptions
- “Light needs vibrating air because it is a wave.” The oscillating quantities are electric and magnetic fields; no material medium is required.
Teaching notes
- Require three mutually perpendicular arrows. Assess spectrum order, not memorized numerical category boundaries.
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14.5 The Doppler Effect
Common misconceptions
- “A moving siren makes sound travel faster through the air.” Ordinary sound speed relative to the air is a medium property; the source changes the spacing of emitted fronts.
Teaching notes
- Use source emission dots separated by equal times; compare moving source with moving observer. Quantitative sound Doppler expressions are enrichment, not required assessment.
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14.6 Wave Interference and Standing Waves
Common misconceptions
- “The second resonance of a closed–open pipe is its second harmonic.” Only odd harmonics fit those boundaries; the second resonance is the third harmonic.
Teaching notes
- Ask students to add displacements at several x values, not just peaks. Diagnose whether pipe diagrams show displacement or pressure.
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14.7 Diffraction
Common misconceptions
- “The central dark minimum has m = 0.” At zero path difference the slit contributions reinforce; the center is bright. Dark minima start at nonzero m.
Teaching notes
- Have students pair the top and bottom halves of a slit at the first minimum. Distinguish single-slit minima from double-slit maxima.
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14.8 Double-Slit Interference and Diffraction Gratings
Common misconceptions
- “Every bright fringe in a real double-slit pattern has equal intensity.” Its finite-width slits supply an envelope that modulates brightness and can remove orders entirely.
Teaching notes
- Ask for both a and d on every sketch. Require sin θ ≤ 1 before accepting a grating order.
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14.9 Thin-Film Interference
Common misconceptions
- “A quarter vacuum wavelength is always the best film thickness.” Use the wavelength inside the coating and inspect both reflection phases. The quarter-wave rule here is λ₀/(4n) for an intermediate-index antireflection layer at normal incidence.
Teaching notes
- Make a two-row interface table first. Complete cancellation requires suitable amplitudes as well as opposite phase; a quarter-wave thickness alone can only minimize reflection.
Unit 15Modern Physics
Build from this unit Practice set Solutions
Topic chapters: Quantum, atomic, and nuclear models
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15.1 Quantum Theory and Wave-Particle Duality
Common misconceptions
- “A massless photon cannot carry momentum.” Zero rest mass does not mean zero energy. A vacuum photon has momentum E/c.
Teaching notes
- Require the student to name the observation that needs the model. Use vacuum photon momentum only unless a different medium model is explicitly provided.
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15.2 The Bohr Model of Atomic Structure
Common misconceptions
- “The number written above the element is the number of neutrons.” A is the total nucleon number. Subtract Z to find neutrons.
Teaching notes
- Ask students to keep separate counts of protons, neutrons, and electrons. Explain that circular Bohr orbits are a model, not a required modern picture of literal electron paths.
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15.3 Emission and Absorption Spectra
Common misconceptions
- “A −3 eV energy level emits a 3 eV photon whenever an electron occupies it.” Emission needs a downward transition; its photon energy is the difference between two levels.
Teaching notes
- Ask which levels are occupied before listing absorption lines. Do not allow “any photon greater than a transition energy works” for a bound-to-bound transition.
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15.4 Blackbody Radiation
Common misconceptions
- “A blackbody emits only at its peak wavelength.” It emits a continuous distribution; Wien’s law locates the greatest spectral contribution, not the only wavelength.
Teaching notes
- Require both peak-position and integrated-area comments on a spectral graph. Do not infer true temperature from an uncalibrated phone photograph’s color.
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15.5 The Photoelectric Effect
Common misconceptions
- “Brighter monochromatic light produces greater stopping voltage.” At fixed frequency it supplies more photons, but maximum electron energy and ideal stopping voltage stay fixed.
Teaching notes
- Require a threshold check before computing Kmax. Ask why the current can change without changing stopping voltage.
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15.6 Compton Scattering
Common misconceptions
- “A Compton photon keeps its momentum because photons always travel at c.” Speed c stays fixed in vacuum, but energy, wavelength, and momentum magnitude can change in the interaction.
Teaching notes
- Use the scattering angle between incoming and outgoing photon directions. Require both momentum components; do not use nonrelativistic electron kinetic energy when recoil is relativistic.
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15.7 Fission, Fusion, and Nuclear Decay
Common misconceptions
- “Exactly half of any small collection must disappear each half-life.” Half-life predicts an expected population fraction. Finite counts fluctuate and individual decay times remain unpredictable.
Teaching notes
- Check all reactants and products, including emitted nucleons. Require a consistent nuclear-mass or atomic-mass convention; ask what the clock predicts for one nucleus versus a sample.
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15.8 Types of Radioactive Decay
Common misconceptions
- “Beta-minus ejects an electron that was already orbiting the atom.” The electron is emitted when a neutron changes into a proton, with an antineutrino; nuclear Z increases.
Teaching notes
- Use electrons and neutrinos with positive lepton number, their antiparticles negative, only for conservation bookkeeping. Do not require neutrino flavors or isotope-pathway memorization.