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Physics 2020 Spring 2009 Stephan LeBohec DATA SHEET - FINAL SEAT # Constants & mathematics: N A =6.02×1023 Boltzmann's constant k =1.38×10−23 J⋅K −1 k= R=8.31 J⋅mol−1⋅K −1 1 9 2 −2 =9.0×10 N⋅m ⋅C 4 0 −7 −1 0=4 ×10 T⋅m⋅A 1 2 Kinetic energy E K = m⋅v 2 cos 2 f t ≈−2 f sin 2 f t t −19 e=1.602×10 C Q Proton =e & Q Electron=−e c= 1 =299,792,458 m⋅s−1≈3×10 8 m⋅s−1 0 0 Work, force & displacement relation ∣⋅ x⋅cos W =∣F sin 2 f t ≈2 f cos 2 f t t Thermodynamics: T K =T C 273 P⋅V =N⋅k⋅T =n⋅R⋅T n= N m = & R=N A⋅k NA M e Actual = 3 Ideal monoatomic gas: U = n⋅R⋅ T 2 Isobaric: W =P V f −V i Isochoric: W =0 Isothermal W =n⋅R⋅T ln First law of thermodynamics: U =Q−W Vf Vi W Cycle QC =1− QH QH 3 Adiabatic: W =− n⋅RT f −T i & 2 P⋅V =Constant 5 with = for monoatomic gases 3 e Carnot =1− TC TH Waves: =c⋅T = c 1 as f = f T In a gas c Sound = Isotropic sound intensity: I = c String = 5 P with = for a monoatomic ideal gas 3 P 2 4 ⋅r Comparing intensities =10 log10 Doppler effect: f o= f s Standing wave frequency (string or open pipe) c f n=n with n=1,2,3,⋯ 2L Electric force, field and potential: Force on a point charge in an electric field: =q E F Electric potential from a point charge: V r =k q r q V R= c±v o c∓v s Standing wave frequency in pipe open at one end c f n=n with n=1,3,5,⋯ 4L Work by operator moving a charge in an electric potential: W =q⋅V f −V i Electric circuits: Power in an electric circuit: P=V⋅I Resistivity: I1 in dB I2 Electric field generated by a point charge: ∣=k q ∣E r2 Force between two point charges: q q ∣=k 1 2 ∣F 2 r Capacitance: C= m F with = L L A Power from harmonic voltage and current: I0 V0 P=I RMS⋅V RMS with I RMS = and V RMS= 2 2 Equivalent resistance for resistors in parallel: 1 1 −1 R Parallel = R 1 R2 Equivalent capacitance for capacitors in series: −1 1 1 C Series = C1 C 2 Electric field in a parallel plate capacitor: ∣= V = ∣E d 0 Energy stored in a capacitor: 1 1 1 q2 2 U = q⋅ V = C⋅ V = 2 2 2C Ohm's law: V =R⋅I Temperature dependence of resistivity: =0 1T −T 0 Equivalent resistance for resistors in series: R Series= R1R 2 Kirchhoff's junction rule: ∑ I IN =∑ I OUT and loop rule: ∑ V UP =∑ V DOWN Equivalent capacitance for capacitors in parallel C Parallel =C 1C 2 Magnetic force and field: ∣=∣q∣⋅∣v∣⋅∣ Magnetic force on a charge: ∣F B∣sin Magnetic field produced by an infinitely long wire: r ∣= 0 I ∣B 2 r Electromagnetic induction: Magnetic flux: = A⋅∣ B∣cos Self inductance: L= Transformers: Magnetic field inside a solenoid: ∣ B∣=0 n I Faraday's law: V =− Induction in a moving wire V =L⋅∣v∣⋅∣ B∣ Mutual inductance: M = ∣=I⋅L∣ Magnetic force on a current: ∣F B∣sin t Induction in a rotating set of coils V =2 f N⋅A⋅∣ B∣sin 2 f t S IP Mutual induction: V =−M I Self induction: V =−L I t I t VS NS IP = = V P NP IS Electromagnetic waves: =c⋅T =c / f Doppler effect: f o= f s 1±v o /c ≈ f s 1±v rel /c 1∓v s /c Reflection of light: Law of reflection: R =I Mirrors equation: Spherical mirror: f = 1 1 1 = f dI dO Magnification: M = Snell's refraction law n1 sin 1 =n2 sin 2 Triangle geometry: µ E b c =a 2b2 cos =b/ c sin =a /c tan =a/b R 2 hI d =− I hO dO Brewster angle: tan B=n 2 / n1 (ABD) and (ECD), similar triangles AB DB AD = = EC DC ED c a Malus law: I T =I I cos 2 D C 2 A B