Formulas2_002 - = ± i R = ρL A(wire P = i± R = R 1 R 2(series q = C±(1-e-t/RC(charging q = q o e-t/RC(discharging 1 R = 1 R 1 1 R 2(parallel

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Constants: e = 1 . 6 × 10 - 19 C m p = 1 . 67 × 10 - 27 kg m e = 9 . 1 × 10 - 31 kg g = 9 . 8 m/s 2 micro = 10 - 6 ǫ o = 8 . 85 × 10 - 12 C 2 /N · m 2 k = 1 / (4 πǫ o ) = 9 × 10 9 N · m 2 /C 2 μ o = 4 π × 10 - 7 T · m/A nano = 10 - 9 Coulomb’s Law: | v F | = | q 1 || q 2 | 4 πǫ o r 2 (point charge) Electric feld: v E = v F q v E = q 4 πǫ o r 2 ˆ r (point charge) v E = i dq 4 πǫ o r 2 ˆ r (general) E = σ 2 ǫ o (plane) Gauss’ law: Φ = ˆ n · v E A = c ˆ n · v E dA = q enc ǫ o Energy: W = i v F · dvs = 1 2 mV 2 f - 1 2 mV 2 i = K f - K i P = v F · vV (mechanical power) For conservative ±orces U f - U i = - i v F · dvs K i + U i = K f + U f Electric potential: ± = U q ± = q 4 πǫ o r (point charge) ± = i dq 4 πǫ o r (general) ± b - ± a = - i b a E x dx = - i b a v E · dvs E x = - ∂± ∂x , E y = - ∂± ∂y , E z = - ∂± ∂z Capacitors: q = C = o A d (parallel-plate) C = C 1 + C 2 (parallel) U = q 2 2 C u = 1 2 ǫ o E 2 1 C = 1 C 1 + 1 C 2 (series) Resistors: i = dq dt = jA R
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Unformatted text preview: = ± i R = ρL A (wire) P = i± R = R 1 + R 2 (series) q = C± (1-e-t/RC ) (charging) q = q o e-t/RC (discharging) 1 R = 1 R 1 + 1 R 2 (parallel) Magnetism: v F = qvV × v B v F = i v L × v B μ = NiA v τ = vμ × v B U =-vμ · v B F l = μ o i 1 i 2 2 πr d v B = μ o 4 π idvs × ˆ r r 2 c v B · dvs = μ o i enc B = μ o i 2 πR , (wire) μ o i 2 R (loop center), μ o iN L (solenoid) 1...
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This note was uploaded on 12/05/2011 for the course PHY 2049 taught by Professor Any during the Spring '08 term at University of Florida.

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