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   Chapter 6Capacitors and Inductors | 
 
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   6.1	Capacitors6.2	Series and Parallel Capacitors6.3	Inductors6.4	Series and Parallel Inductors | 
 
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   A capacitor is a passive element designed        to store energy in its electric
       field. | 
 
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   Capacitance C is the ratio of the charge q on one plate of a capacitor
       to the voltage difference v between the two plates, measured in farads
       (F). | 
 
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   If i is flowing into the +ve terminal of C
    Charging => i is +veDischarging => i is –ve 
 | 
 
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   The energy, w, stored in the capacitor is | 
 
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   Example 1
 
 
    The current through a 100-mF
        capacitor is
 
 i(t) = 50 sin(120 pt) mA.
 
 Calculate the voltage across it at t =1 ms andt = 5 ms.
 
 Take v(0) =0. 
 | 
 
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   Example 2
 
 
    An initially uncharged 1-mF capacitor has the current shown below
        across it.
 
 Calculate the voltage across it at t = 2 ms andt = 5 ms. 
 | 
 
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   The equivalent capacitance of N parallel-connected capacitors is the sum
       of the individual capacitances. | 
 
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   The equivalent capacitance of N series-connected capacitors is the
       reciprocal of the sum of the reciprocals of the individual capacitances. | 
 
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   Example 3 Find the equivalent capacitance
       seen at the terminals of the circuit in the circuit shown below:
 
 | 
 
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   Example 4Find the voltage across each of the capacitors in the circuit shown
       below:
 
 | 
 
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   An inductor is a passive element designed         to store energy in its magnetic
       field. | 
 
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   Inductance is the property whereby an inductor exhibits opposition to
       the change of current flowing through it, measured in henrys (H). | 
 
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   The current-voltage relationship of an inductor: | 
 
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   Example 5	The terminal voltage of a 2-H   
       inductor is Find the current flowing through
       it at    t = 4 s and the energy
       stored in it within 0 < t < 4 s.
 
 	Assume i(0) = 2 A. | 
 
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   Example 6
 
 	Determine vc, iL, and the energy stored in the
       capacitor and inductor in the circuit of circuit shown below under dc
       conditions. | 
 
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   The equivalent inductance of series-connected inductors is the sum of
       the individual inductances. | 
 
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   The equivalent capacitance of parallel inductors is the reciprocal of
       the sum of the reciprocals of the individual inductances. | 
 
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   Example 7	Calculate the equivalent inductance for the inductive ladder network in
       the circuit          shown below:
 
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   Current and voltage relationship for R, L, C
 
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