Find current at high/low frequency

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SUMMARY

The discussion focuses on calculating the RMS current delivered by a 45V (RMS) power supply at varying frequencies. For very high frequency, the RMS current is determined to be 225mA, while at very low frequency, it is 450mA. The analysis relies on the impedance characteristics of inductors and capacitors, where the impedance of the inductor approaches infinity at high frequencies and the impedance of the capacitor approaches infinity at low frequencies, simplifying the circuit analysis.

PREREQUISITES
  • Understanding of RMS voltage and current calculations
  • Knowledge of impedance in AC circuits
  • Familiarity with inductors and capacitors in electrical engineering
  • Basic grasp of complex numbers and their application in circuit analysis
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  • Study the concept of impedance in AC circuits, focusing on inductors and capacitors
  • Learn about the relationship between frequency and impedance in electrical components
  • Explore the use of complex numbers in circuit analysis
  • Investigate the implications of high and low frequency on circuit behavior
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Electrical engineering students, circuit designers, and anyone interested in understanding the behavior of AC circuits at varying frequencies.

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Homework Statement


find the rms current delievered by the 45v (rms) power supply when
a) the frequency is very large
and b) the frequency is very small.

answer: a) 225mA, b) 450mA

http://yfrog.com/jucurrentqg

http://img714.imageshack.us/img714/1592/currentq.gif

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Homework Equations


w= angular velocity (supposed to be omega)
L= inductor
C= capacitor
j= complex coefficient = sqrt(-1)
Zl= resistance of inductor
Zc= resistance of capacitor
Ztot= total resistance
R= resistance of resistor
P= Power

Xl=wL
Xc=1/wc
Zl=j*Xl
Zc=-j*Xc
Ztot= R + Zl + Zc = R + j(Xl-Xc)



The Attempt at a Solution



with frequency just being high, how am I supposed to get these exact numbers without letters/symbol for I? o.o I tried the calculation and omega did not cancel out either.
 
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The key idea is that in the case of very high or very low frequency, you can take the impedance (resistance) of the inductor and capacitor to be ~infinite, respectively. Does it make sense why that's true (as an approximation at least)?

In effect, this eliminates one of the two loops in the circuit for each case.
 
zhermes said:
The key idea is that in the case of very high or very low frequency, you can take the impedance (resistance) of the inductor and capacitor to be ~infinite, respectively. Does it make sense why that's true (as an approximation at least)?

In effect, this eliminates one of the two loops in the circuit for each case.

ah yes it does, at first I thought the resistance would skyrocket to infinity / 0
thank you
 
Last edited:

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