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Page Title: Figure 2 Coil Circuit and Phasor Diagram
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Voltage and Current Phase Relationships in an Inductive Circuit
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Electrical Science Volume 3 of 4
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Inductive Reactance Summary

Basic AC Reactive Components INDUCTANCE According  to  Lenz’s  Law  (refer  to  Module  1,  Basic  Electrical  Theory),  the  induced  voltage always opposes the change in current.   Referring to Figure 1, with the current at its maximum negative value (point a), the induced EMF is at a zero value and falling.  Thus, when the current rises in a positive direction (point a to point c), the induced EMF is of opposite polarity to the applied voltage and opposes the rise in current.  Notice that as the current passes through its zero value (point b) the induced voltage reaches its maximum negative value.   With the current now at its maximum positive value (point c), the induced EMF is at a zero value and rising.   As the current is falling toward its zero value at 180° (point c to point d), the induced EMF is of the same polarity as the current and tends to keep the current from falling.  When the current reaches a  zero  value,  the  induced  EMF  is  at  its  maximum  positive  value.   Later,  when  the  current  is increasing  from  zero  to  its  maximum  negative  value  at  360°  (point  d  to  point  e),  the  induced voltage is of the opposite polarity as the current and tends to keep the current from increasing in the negative direction.   Thus, the induced EMF can be seen to lag the current by 90°. The value of the self-induced EMF varies as a sine wave and lags the current by 90°, as shown in  Figure  1.   The  applied  voltage  must  be  equal  and  opposite  to  the  self-induced  EMF  at  all times; therefore, the current lags the applied voltage by 90° in a purely inductive circuit. If  the  applied  voltage  (E)  is  represented  by  a  vector  rotating  in  a  counterclockwise  direction (Figure 1b), then the current can be expressed as a vector that is lagging the applied voltage by 90°.   Diagrams of this type are referred to as phasor diagrams. Example: A  0.4  H  coil  with  negligible  resistance  is  connected  to  a  115V,  60  Hz  power source  (see  Figure  2).   Find  the  inductive  reactance  of  the  coil  and  the  current through  the  circuit.    Draw  a  phasor  diagram  showing  the  phase  relationship between current and applied voltage. Figure 2   Coil Circuit and Phasor Diagram Rev. 0 Page 3 ES-08

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