I=V/R R=V/I |
Assuming the incoming current to be positive and outgoing current negative we have I e incoming current = ∑ outgoing current thus, the above Law can also be stated as the sum of current flowing towards any junction in an electric circuit is equal to the sum of currents flowing away from that junction |
Suppose that a current i flows through the external resistance (8 Ω) and it divides Using KCL , i1 + i2 = i |
Using KVL, For Loop ABYXA : 10 + (−i1)1 + (i − i1) 1 − 8 = 0 For Loop ABQPA : 10 + (−i1)1 + (−i)8 = 0 Solving, we get, i = 18/17 A ≈ 1.06A i1 = 10 − 8i = (10 − 8.54)A = 1.52 A. = − 0.46 A |
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Ra = R9 x (R8 + R10)/ R9 + R8 + R10 = 6 x (10+2)/ 6 + 10 +2 = 4 Ω |
Rb = R6 x(Ra + R7)/ R5 + Ra + R7 = 6 x (4 +8) / 6 +4 +8 = 4Ω |
Rc = R4 x (RB + R5) / R4 + RB + R5 = 8 x (4 + 4) / 8 + 4 + 4 = 4 Ω |
Rd = R2 x (Rc + R3)/ R2 + Rc + R3 = 8 x (4 + 4) / 8 + 4 + 4 = 4 Ω |
N/60 = n P/2 = p |
The RMS value of AC current is equal to the steady state DC current that required to produce the same amount of heat produced by ac current provided that resistance and time for which these currents flows are identical I rms = |
= For the derivation we are considering only hall cycle. Thus varies from 0 to ᴫ i = Im Sin Solving We get Similarly, Vavg= |
It is opposition to the flow of an AC current offered by the inductor. XL = ω L But ω = 2 ᴫ F XL = 2 ᴫ F L It is measured in ohm XL∝FInductor blocks AC supply and passes dc supply zero
2. Capacitive Reactance (Xc) It is opposition to the flow of ac current offered by the capacitor Xc = Measured in ohm Capacitor offers infinite opposition to dc supply
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Impedance (Z) The ac circuit is to always pure R Pure L and pure C it well attains the combination of these elements. “The combination of R1 XL and XC is defined and called as impedance represented as Z = R +i X Ø = 0 only magnitude R = Resistance, i = denoted complex variable, X =Reactance XL or Xc | |||
Polar Form Z = L I Where = Measured in ohm | |||
It is the cosine of the angle between voltage and current If Ɵis –ve or lagging (I lags V) then lagging P.F. If Ɵ is +ve or leading (I leads V) then leading P.F. |
Consider pure Inductor (L) is connected across alternating voltage. Source V = Vm Sin ωt When an alternating current flow through inductance it setups alternating magnetic flux around the inductor. This changing the flux links the coil and self-induced emf is produced According to faradays Law of E M I | ||||
e = | ||||
at all instant applied voltage V is equal and opposite to self-induced emf [ Lenz's law] V = -e = But V = Vm Sin ωt
dt Taking integrating on both sides dt dt (-cos ) but sin (– ) = sin (+ ) sin ( - /2) And Im=
/2) /2 = -ve = lagging = I lag v by 900
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Power P = Ѵ. I = Vm sin wt Im sin (wt /2) = Vm Im Sin wt Sin (wt – /s) ① And Sin (wt - /s) = - cos wt ② | |
Sin (wt – ) = - cos sin 2 wt from ① and ② The average value of sin curve over a complete cycle is always zero Pavg = 0
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