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Phys 102 – Lect. 29 Final exam review 1 Final exam study approaches How should you study for the physics exam? • Cramming DOES NOT work • Emphasize understanding concepts & problem solving, NOT memorization • Review pre-lecture & lecture concepts • Review problems: ACTs, HW, quizzes, practice exams • Understand formula sheet (i.e. when to use and when NOT to use an eq.) & know what each symbol means • Do practice exam problems (time yourself!) Phys. 102, Review 29, Slide 2 Review lecture ACTs Some exam problems are inspired by ACTs. EX2 30% 70% Phys. 102, Review 29, Slide 3 Review homework questions Some exam problems are inspired by the HW. EX2 20%! 100% Phys. 102, Review 29, Slide 4 Problem solving approaches The not-so-good approaches: EX2 “Reasoning by analogy”/memorization: “I remember every time we’ve done RC circuit problems, VC = after a long time...” The good approach: Conceptual understanding / reasoning from basic principles: 20%! 1. 2. 3. 4. The capacitor is fully charged, so IC = 0 Resistor R3 is in series with C so I3 = 0 But, current can flow around inner loop, so I1 > 0 Algebra! KLR: – I1R1 – VC = 0, therefore VC < Phys. 102, Review 29, Slide 5 Problem solving approaches The not-so-good approaches: EX2 The “magic” equation: “What equation will solve this problem? Req = R1+R2, V = IR?” The good approach: Conceptual understanding / reasoning from basic principles: 70% 1. 2. 3. 4. Redraw the circuit to make it clearer The rightmost resistor is shorted, so no current flows through it! So, the current through the bottom resistor is I Algebra! KLR: E – IR = 0 Phys. 102, Review 29, Slide 6 1. Electricity & circuits Lects. 1 – 9 7 Relationship between F, E, UE, V Vector F Number (“scalar”) UE [N] Ex: F k q1q2 r2 WE F r cos θ U E Ex: U k V [N/C]=[V/m] Ex: E k q1q2 r V UE q EF q E [J] q r2 E points from high to low V [J/C]=[V] Ex: V k q r Phys. 102, Review 29, Slide 8 Circuits & components Wire Battery Series and parallel 2 V1 V2 Veq Iin Iout Current In = Current Out 2 I1 I 2 I eq Resistor Basic principles: Conservation of charge (KJR) Conservation of energy (KLR) 1 1 Capacitor I1 I 2 I eq V1 V2 Veq V 0 Sum of voltages around loop = 0 Phys. 102, Review 29, Slide 9 RC Circuits Charging: Discharging: Initially the capacitor is uncharged At t = 0 we close switch S1 Initially the capacitor is fully charged At t = 0 we close switch S2 Immediately after (t = 0): No charge on C yet Current IC,0 flows charge onto C Immediately after (t = 0): C still fully charged Current IC,0 flows charge off of C VC ,0 Q 0 0 I C ,0 0 C ε C acts like a wire After a long time (t = ): Charge on C builds and saturates Current decreases to zero VC , Q 0 C R + I C , 0 C acts like an open circuit +Q –Q S1 VC ,0 IC C acts like a battery C S2 Q0 0 I C ,0 0 C After a long time (t = ): Charge dissipates to zero Current decreases to zero VC , Q 0 C I C , 0 C acts like an open circuit Phys. 102, Review 29, Slide 10 2. Magnetism Lects. 10 – 15 11 B Magnetism summary Type I: RHR for forces on moving charges and currents Type II: RHR for magnetic fields generated by currents B field from wire Moving + charges and currents v I + Moving – charges v q q F Thumb along v Fingers along B F on + q is out of palm F q vB sin θ – I B B I I B F F B field inside loop B B I B I Thumb along v Fingers along B F on – q is into palm F ILB sin θ τloop NIAB sin θ μB sin θ Thumb along I Curl fingers along I Curl fingers along B Thumb along B Bwire μ0 I 2πr OR: Thumb along I Curl fingers along B Bsol μ0 nI Phys. 102, Review 29, Slide 12 Lenz law Induced EMF ε opposes change in flux 1. Is increasing, decreasing, or constant? 2. If increases: ε induces B field opposite external B field If decreases: ε induces B field along external B field Bext Bext Bext Bext I Bind Bind I Bind I Bind I Top view Top view Side view Side view If is constant: ε is zero, no induced B field Bind I 3. Type II RHR gives current direction Curl fingers along I Thumb along Bind I Bind Phys. 102, Review 29, Slide 13 Faraday’s law Faraday’s law: “Induced EMF” = rate of change of magnetic flux ε t Since BA cos φ, 3 things can change 1. Area of loop 2. Magnetic field B 3. Angle φ B(t) v +1.0 B ω n +0.5 0 B t 0 10 20 -0.5 ε BLv -1.0 ε B A t ε (t ) ωNBA sin ωt Phys. 102, Review 29, Slide 14 3. Light & optics Lects. 16 – 23 15 Light summary Properties of electromagnetic waves Relation between E, B, f, λ Energy density, power & intensity Polarization Itrans Iinc cos2 θ I P A 2 c utot cε0 Erms Ray model of light Reflection θi θr Refraction n1 sin θ1 n2 sin θ2 1 1 1 Mirrors f d o di Lenses (alone, in combination) The eye (nearsightedness, farsightedness) m hi d i ho do Interference Constructive and destructive interference Diffraction & resolution Phys. 102, Review 29, Slide 16 Light as a wave (again) Interference: phase shift & path length difference θ θ Phase shift d Constructive: phase shift of mλ Destructive: phase shift of (m + ½)λ Two & multiple slit maxima d sin θm mλ Two slit minima d sin θm (m 1 )λ 2 θ d sin θ m 0, 1, 2... Single slit minima a sin θm mλ m 1, 2... Circular aperture minimum D sin θ1 1.22 λ Phys. 102, Review 29, Slide 17 Example: Interference Extra practice Phys. 102, Review 29, Slide 18 4. Modern physics Lects. 23 – 28 19 Quantum mechanics Wave-particle duality Matter waves – particle as a wave (de Broglie) Photons – light as a particle (photoelectric effect) λ h p Bohr model quantized orbits & energies, electronic transitions n2 Z2 rn a0 En 13.6eV 2 Z n Quantum model quantum numbers (n, ℓ, mℓ, ms), Pauli exclusion principle, magnetic properties of atoms Nuclear & particle physics structure of nucleus & nucleons decay processes (α, β, γ) & rates, binding energy quark model Phys. 102, Review 29, Slide 20 Example: wave-particle duality Extra practice Phys. 102, Review 29, Slide 21 Example: quantum numbers Extra practice Phys. 102, Review 29, Slide 22 Example: quantum atom Extra practice Phys. 102, Review 29, Slide 23 Example: nuclear decay Extra practice Phys. 102, Review 29, Slide 24