The series of alternating current
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The series of alternating current. 1.10 Purely Series Barriers 10/02 Series Inductive Obstacles An inductor coil has a self inductance L coupled alternating voltage V, then the resulting emf induction coil ujung2 Barriers have inductive XL price: XL = inductive resistance (Ohm).

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The series of alternating current

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The series of alternating current

The series of alternating current


The series of alternating current

1.10 Purely Series Barriers10/02 Series Inductive ObstaclesAn inductor coil has a self inductance L coupled alternating voltage V, then the resulting emf induction coil ujung2Barriers have inductive XL price:XL = inductive resistance (Ohm)


The series of alternating current

3.10 Barriers Series CapacitanceA capacitor with capacity C connected alternating voltage V, then the capacitor becomes charged, so that at plat2nya have a potential difference ofLarge capacitive barrier XC:


The series of alternating current

10.4 The series R-L SeriesBarriers to R and XL series connected dg TEG. alternating V.Ohm's Law I:VR = potential difference between ujung2 RVL = the potential difference between ujung2 XLLarge total voltage V is written in a vector:

Resistance R and XL also summed in the vector:Z = Impedance (Ohm)

Strong currents which flow in this circuit are:


The series of alternating current

5.10 The series of R-C SeriesBarriers to R and XC series connected dg TEG. alternating V.Ohm's Law I:VR = potential difference between ujung2 RVC = potential difference between ujung2 XCLarge total voltage V is written in a vector:

Resistance R and XC are also summed in the vector:Z = Impedance (Ohm)

Strong currents which flow in this circuit are:


The series of alternating current

6.10 The series of R-L-C SeriesBarriers series R, XL and XC are connected dg TEG. alternating V.Ohm's Law I: VR = potential difference between ujung2 R VC = potential difference between ujung2 XC VL = the potential difference between ujung2 XL Large total voltage V is written in a vector:esistance R, XL and XC are also summed in the vector:Z = Impedance (Ohm)

Strong currents which flow in this circuit are:


The series of alternating current

10.7 Series ResonanceIf the RLC series circuit then XL = XCEffective flow in the circuit will achieve the greatest price that is atIt said circuit in a state of resonance. In this case appliesSo the resonant frequency is


The series of alternating current

  • The relationship between the maximum and effective priceVef = effective voltage (V) Vm = maximum voltage (V) ief = effective current (A) im = maximum current (A)The relationship between price and average maximumVr = average voltage (V) Vm = maximum voltage (V) ir = average current (A) im = maximum current (A)


The series of alternating current

10.8 Power Flow Back and forthFormulated in direct current power P = VI, with V and i the price is always fixed.But for alternating current electric power is expressed as: multiplication of voltages, currents and power factor.

By:P = electrical power back and forth (Watt)V = effective voltage (V)i = effective strong currents (A)Z = impedance circuit (Ohm)Cos θ = power factor =


The series of alternating current

Example:Jala2 have a different mains voltage 220 V, what is the maximum voltage value?In a series RLC circuit with R = 80 Ohm, XL = 100 Ohm, and XC = 40 Ohm, connected by alternating voltage source having a maximum voltage of 120 V. Determine the maximum current in the circuit.At frequency of 100 Hz, the reactance of a capacitor is 4000 ohms and reactance of an inductor is 1000 Ohm. If the capacitors and inductors were mounted on a circuit, the resonance occurs at what frequency?In a series RLC circuit with R = 40 Ohm, XL = 50 Ohm, and XC = 20 Ohm, connected by alternating voltage source having an effective voltage of 110 V. Determine the power used by the entire circuit.


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