RLC Circuits: Current from Emf at Very Large/Small Freq.

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Homework Help Overview

The original poster is inquiring about the current supplied by an emf in an RLC circuit at very high and very low frequencies. The circuit consists of resistors, an inductor, and a capacitor, with specific values provided for each component.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the behavior of inductors and capacitors at extreme frequencies, questioning how these components react to rapidly changing versus nearly constant voltages. There is also a focus on the configuration of the circuit components and their implications for the problem.

Discussion Status

Some participants have offered insights into the behavior of circuit elements at different frequencies, prompting further exploration of the circuit's configuration. There is ongoing clarification regarding the arrangement of components and their respective roles in the circuit.

Contextual Notes

The original poster notes the absence of a specific frequency value, which may impact the analysis. Additionally, there is a question about whether certain resistances are in series with the capacitor or represent capacitive reactance, indicating potential assumptions that need to be examined.

kevin7913
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Homework Statement


What is the current supplied by the emf when the frequency is very large and very small?

-------------------------
| |
| ------------------------
| | |
| 100ohm 50ohm
10Vrms | |
| 50mH 20*10^-6F
| | |
| ------------------------
| |
|--------------------------

Homework Equations


Vrms =v/2^(1/2), Z=(R^2 + (XL - Xc)^2)^(1/2), VR =IR, VL =IXL, Vc=IXc

The Attempt at a Solution



I don't know where to start, since they didn't give the frequency.
Please help
 
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the picture didn't shows up very good, it's a 100ohm and a 50mH in series and parrell with a 50ohm and a 20*10^-6F in series
 
HTML ignores consecutive whitespace.
Using the quote feature, I was able to get your circuit.
Surround by
Code:
 [/ code] (no space in the tag)

crudely,
[code]

[FONT="Arial"]
-------------------------
|                                 |
|                  ------------------------ 
|                  |                               | 
|             100ohm                         50ohm
10Vrms          |                               |
|              50mH                             20*10^-6F
|                  |                               |
|                  ------------------------
|                                   |
|--------------------------
 
Forget equations. Think about how you can replace the capacitor and inductor at high enough and low enough frequencies (ie the limits as f->0 and f->infinity)
 
Last edited:
If the frequency is very high, the supplied voltage is rapidly changing. How does the inductor behave in response to this rapidly changing emf?

If the frequency is very low, the supplied voltage can be approximated as nearly constant over a finite interval of time. How does the inductor behave as a result of this nearly constant source?

Now go back and consider what the capacitor is doing in both cases.
 
Whether the 50 ohm resistance is connected in series with the capacitor or is it the capacitive reactance of the capacitor?
 
rl.bhat said:
Whether the 50 ohm resistance is connected in series with the capacitor or is it the capacitive reactance of the capacitor?

I believe they are in series, as the capacitive reactance depends on the frequency of the source. By giving the resistance as a definitive 50 ohms, it seems to be implied that it does not depend on the frequency of the emf.
 

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