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Lesson 4-1 Introduction to Direct-Current RL Circuits

Introduction to DC RL Circuits

The Phantom Circuit  

 

You will rarely find a circuit that is actually made up of a 
resistor and inductor connected in series with a DC source. However, such circuits exist in abundance and  in various disguises such as DC motors,  relays, and electromagnets--any circuit that has a DC current passing through a coil of wire. 

Where is the resistor in these examples? There may or may not be an actual resistor connected in series with the coil of 

wire; but even if there is not, there is still the resistance of the coil of wire, itself. 

Series RL circuits are most often equivalent circuits, or circuits that present a simplified and more manageable view of an actual circuit. 

Looking at such circuits as a simple series RL circuit can help you understand how such circuits operate and how best to go about designing, analyzing, and troubleshooting them.

Before starting this module, you should be able to: When you complete this module, you should be able to: 
  • Describe how inductors oppose any change in current flowing through them.
  • Cite the units of measure for inductance.
  • Determine how much energy is stored in the magnetic field around an inductor that is carrying a DC current.
  • Describe the meaning of build-up current for a series RL circuit.
  • Describe the meaning of decay current for a series RL circuit.

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Energy Stored in a Magentic Field 
 
  • Current flows through a series RL circuit when a DC voltage is applied to it. 
  • Current flowing through a series RL circuit causes the inductor to create a magnetic field. 
  • Energy is stored in the magnetic field surrounding a current-carrying inductor. 

The amount of energy stored in the magnetic field of an inductor is given by:  

 

where:  

    E = the amount of stored energy in joules  
    L = inductance in henries  
    I = current in amperes  
     

The magnetic field surrounding an inductor is present only as long as current is flowing through the inductor. 

The amount of current flowing through the inductor in a series RL circuit is determined by the values of the voltage source (VS) and the resistor (R): 

I = VS/R



The amount of energy stored in the magnetic field surrounding an inductor is: 

  • Proportional to the value of the inductor.
Doubling the value of the inductor doubles the amount of stored energy.
  • Proportional to the square of the current through the inductor.
Doubling the amount of current quadruples the amount of stored energy.

 

P
R
E
V
I
E
W
Build-Up Current 

When DC power is first applied to a series RL circuit, the self-inductance effect opposes the build-up of current flow.  Current gradually increases, however, and eventually reaches a point where there is no longer any change in the current level and, therefore, no further self-inductance effect. 
 

Energy is stored in the magnetic field as long as current continues to flow through the inductor.

 
 
 
 

 

 
 
 

P
R
E
V
I
E
W

Decay Current 

When DC power is removed from a series RL circuit, the magnetic field that had been built up around the inductor begins to collapse. There is no longer a source of energy to sustain it. 

As the field collapses, its lines of force induce a current that tends to keep current flowing through the circuit. Energy that had been stored in the magnetic field is converted to electrical energy. 

There is a limited amount of energy stored in the magnetic field, so the induced current gradually decreases to zero. 

Energy that had been stored in the magnetic field when DC power was applied to the circuit is transformed into electrical energy when the DC power source is removed. 

 

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Author and Content Provider: David L. Heiserman
Publisher: SweetHaven Publishing Services

Copyright © 1997, 2003, 2005 David L. Heiserman
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