Midterm 1 phy303l

# Midterm 1 phy303l - midterm 01 DAVIS LINDSY Due 11:00 pm 1...

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midterm 01 – DAVIS, LINDSY – Due: Feb 14 2008, 11:00 pm 1 Electric force and electric Feld Electric force between 2 point charges: | F | = k | q 1 || q 2 | r 2 k = 8 . 987551787 × 10 9 N m 2 /C 2 ǫ 0 = 1 4 π k = 8 . 854187817 × 10 12 C 2 /N m 2 q p = q e = 1 . 60217733 (49) × 10 19 C m p = 1 . 672623 (10) × 10 27 kg m e = 9 . 1093897 (54) × 10 31 kg Electric Feld: v E = v F q Point charge: | E | = k | Q | r 2 , v E = v E 1 + v E 2 + ··· ±ield patterns: point charge, dipole, b plates, rod, spheres, cylinders, ... Charge distributions: Linear charge density: λ = Δ Q Δ x Area charge density: σ A = Δ Q Δ A Surface charge density: σ surf = Δ Q surf Δ A Volume charge density: ρ = Δ Q Δ V Electric ²ux and Gauss’ law ±lux: ΔΦ = E Δ A = v E · ˆ n Δ A Gauss law: Outgoing Flux from S, Φ S = Q enclosed ǫ 0 Steps: to obtain electric ±eld –Inspect v E pattern and construct S –Find Φ s = c surface v E · d v A = Q encl ǫ 0 , solve for v E Spherical: Φ s = 4 π r 2 E Cylindrical: Φ s = 2 π r ℓE Pill box: Φ s = E Δ A , 1 side; = 2 E Δ A , 2 sides Conductor: v E in = 0, E b surf = 0, E surf = σ surf ǫ 0 Potential Potential energy: Δ U = q Δ V 1 eV 1 . 6 × 10 19 J Positive charge moves from high V to low V Point charge: V = k Q r V = V 1 + V 2 = ... Energy of a charge-pair: U = k q 1 q 2 r 12 Potential di³erence: | Δ V | = | E Δ s b | , Δ V = v E · Δ vs , V B V A = i B A v E · dvs E = d V dr , E x = Δ V Δ x v v v fix y,z = ∂V ∂x , etc. Capacitances Q = C V Series: V = Q C eq = Q C 1 + Q C 2 + Q C 3 + ··· , Q = Q i Parallel: Q = C eq V = C 1 V + C 2 V + ··· , V = V i Parallel plate-capacitor: C = Q V = Q E d = ǫ 0 A d Energy: U = i Q 0 V dq = 1 2 Q 2 C , u = 1 2 ǫ 0 E 2 Dielectrics: C = κC 0 , U κ = 1 2 κ Q 2 C 0 , u κ = 1 2 ǫ 0 κE 2 κ Spherical capacitor: V = Q 4 π ǫ 0 r 1 Q 4 π ǫ 0 r 2 Potential energy: U = v p · v E Current and resistance Current: I = d Q dt = nq ± d A Ohm’s law: V = I R , E = ρJ E = V , J = I A , R = ρℓ A Power: P = I V = V 2 R = I 2 R Thermal coe´cient of ρ : α = Δ ρ ρ 0 Δ T Motion of free electrons in an ideal conductor: = ± d q E m τ = J n q ρ = m n q 2 τ Direct current circuits V = I R Series: V = I R eq = I R 1 + I R 2 + I R 3 + ··· , I = I i Parallel: I = V R eq = V R 1 + V R 2 + V R 3 + ··· , V = V i Steps: in application of Kirchho²’s Rules –Label currents: i 1 ,i 2 ,i 3 ,... –Node equations: i in = i out –Loop equations: ( ±E ) + ( iR )=0” –Natural: “+” for loop-arrow entering terminal ” for loop-arrow-parallel to current ³ow RC circuit: if d y dt + 1 R C y = 0, y = y 0 exp( t R C ) Charging: E − V c Ri = 0, 1 c d q dt + R d i dt = i c + R d i dt = 0 Discharge: 0 = V c R i = q c + R d q dt , i c + R d i dt = 0 Magnetic Feld and magnetic force μ 0 = 4 π × 10 7

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Midterm 1 phy303l - midterm 01 DAVIS LINDSY Due 11:00 pm 1...

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