Home  www.playhookey.com  Sat, 06242017 

Direct Current

Alternating Current

Semiconductors

Digital

Logic Families

Digital Experiments

Computers

 Analog  Analog Experiments  Oscillators  Optics  HTML Test  

 The Fundamentals  Resistance and Reactance  Filter Concepts  Power Supplies   

Series RC Circuits

Series RL Circuits

Parallel RC Circuits

Parallel RL Circuits

 Series LC Circuits  Series RLC Circuits  Parallel LC Circuits  Parallel RLC Circuits   AC Applications of the Wheatstone Bridge  
Parallel RL Circuits 

With an ac signal applied to it, the parallel RL circuit shown to the right offers a significant impedance to the flow of current. This impedance will change with frequency, since that helps determine X_{L}, but for any given frequency, it will not change over time.
As you would expect, Ohm's Law still applies, just as it has in other circuits. Voltage, being the same for all components, is our reference. Current, however, is the sum of the currents through R and L, keeping in mind that the coil opposes any change in current through itself, so its current lags behind its voltage by 90°. Therefore, our basic equation for current must be:
I =  V  =  V   j  V 




Z  R  X_{L} 
If we move the "j" to the denominator of its fraction, we must change its sign. This is also in keeping with the fact that jωL = jX_{L}. As with the parallel RC circuit, we can divide the entire equation by V and solve for the complex impedance of this circuit. Our resulting initial equation is:
1  =  1  +  1 




Z  R  jX_{L} 
To calculate the total circuit impedance, we go back to the general equation that we introduced when discussing RC parallel circuits:
Z  =  R × j(X_{L}  X_{C}) 


R + j(X_{L}  X_{C}) 
This time, however, we only have R and L, so the X_{C} factors drop out of the equation. This leaves us with:
Z  =  R × (jX_{L}) 


R + jX_{L} 
We complete the calculation using the same relationship we applied with the parallel RC circuit, to remove the "j" from the denominator:
Z  =  R × jX_{L}  ×  R  jX_{L} 



R + jX_{L}  R  jX_{L}  
=  (jRX_{L})(R  jX_{L})  


(R + jX_{L})(R  jX_{L})  
=  jR²X_{L}  j²RX_{L}²  


R² + X_{L}²  
=  RX_{L}² + jR²X_{L}  


R² + X_{L}² 
As before, this gives us an entirely real number in the demoninator, which in turn makes the necessary computations possible and practical. Our parallel RL impedance is still a complex number, which can be written as:
Z  =  RX_{L}²  + j  R²X_{L} 



R² + X_{L}²  R² + X_{L}² 
This expression can now be used to calculate the parallel impedance of any resistor and any inductor, provided the signal frequency is known. If you wish to attempt the same sort of proof that we used for the parallel RC circuit, you will find that your results still match exactly.


 
All pages on www.playhookey.com copyright © 1996, 20002015 by
Ken Bigelow Please address queries and suggestions to: webmaster@playhookey.com 