CC0929 Semester 2, 2017 Page 1 of 3 PHYS1003 Physics 1 (Technological) Formula Sheet Fluids ρ = m V p = F A p = nRT V = NkT V pgauge = p− p0 Q = dV dt = Av A1v1 = A2v2 p1 + ρgy1 + 1 2 ρv21 = p2 + ρgy2 + 1 2 ρv22 F = ηAv L Q = dV dt = pi∆pR4 8ηL Re = ρvL η FD = 6piηrv FD = 1 2 ρACDv 2 Quantum Physics E = hf hf = Kmax + Φ p = hf c = h λ L = √ l(l + 1)~ ∆λ = h mc (1− cosφ) S = √ 3 4 ~ λ = h p = h mv ~ = h 2pi − ~ 2 2m d2ψ dx2 + Uψ = Eψ λ = 2L n for n = 1, 2, 3 . . . ∆x∆px ≥ ~/2, ∆y∆py ≥ ~/2, ∆z∆pz ≥ ~/2 +∞∫ −∞ |ψ(x)|2dx = 1 En = ( h2 8mL2 ) n2 for n = 1, 2, 3 . . . hf = hc λ = Ei − Ef ψn(x) = A sin (npi L x ) for n = 1, 2, 3 . . . 1 λ = RH ( 1 n2lower − 1 n2upper ) En = − me 4 8ε02h2n2 = −13.60 n2 eV for n = 1, 2, 3 . . . λmT = 2.90× 10−3 m.K k = √ 2m(U0 − E) ~ U = −→µ · −→B sin θ = mλ 2d 1 CC0929 Semester 2, 2017 Page 2 of 3 Electricity & Magnetism/Circuits F = |q1q2| 4piε0r2 −→ F = q( −→ E +−→v ×−→B ) −→ E = −→ F q0 ΦB = ∫ B cosφdA = ∫ −→ B · d−→A ΦE = ∫ E cos θdA = ∫ −→ E · d−→A ∮ −→ B · d−→A = 0∮ −→ E · d−→A = Qencl ε0 R = mv |q|B V = U q −→ F = i −→ l ×−→B V = 1 4piε0 ∑ i qi ri Va − Vb = b∫ a −→ E · d−→l C = Q Vab = ε0 A d (parallel plates) B = µ0I 2pir (straight wire) U = Q2 2C = 1 2 CV 2 = 1 2 QV F L = µ0II ′ 2pir K = C C0 E = E0 K I = dQ dt ∮ −→ B · d−→l = µ0Iencl −→ J = nq−→vd B = µ0NI L (solenoid) ρ = E J ε = −N dΦB dt R = ρL A ε = vBL P = V I = I2R = V 2 R ∮ −→ E · d−→l = −dΦB dt ε = −Ldi dt L = NΦB i U = 1 2 LI2 VR = IR, VL = IXL, VC = IXC q = Cε ( 1− e−t/RC ) q = Q0e−t/RC ω = 1√ LC τ = RC 2 CC0929 Semester 2, 2017 Page 3 of 3 Electricity & Magnetism/Circuits (continued) τ = L R Rtotal = R1 +R2 vout = vinR2 R1 +R2 1 Rtotal = 1 R1 + 1 R2 v = V0ejωt = V0 cos (ωt) + jV0 sin (ωt) XC = 1 ωC v = Zi XL = ωL Q = f0 f2 − f1 Ztotal = Z1 + Z2 vout = vinZ2 Z1 + Z2 1 Ztotal = 1 Z1 + 1 Z2 ω = 2pif F = ma (vx)f = (vx)i + ax∆t xf = xi + (vx)i∆t+ 1 2 ax(∆t)2 (vx)2f = (vx) 2 i + 2ax∆x 3
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