Solving circuit using complex numbers

AI Thread Summary
The discussion focuses on solving a circuit problem involving complex numbers, specifically finding the current when given resistance (R), inductive reactance (X_L), capacitive reactance (X_C), and a sinusoidal voltage source. The voltage is expressed in phasor form, and the relationship between voltage and current is established using complex impedances. There is confusion regarding the interpretation of R, X_L, and X_C, with clarification needed on their roles in the circuit. Participants emphasize the importance of using complex impedances to derive the total current as a function of the given parameters. The conversation highlights the need for proper notation and understanding of circuit components to solve the problem effectively.
masterjoda
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Homework Statement


Find the current in them in this circuit, if we know R=X_L, X_C and u=5sin(314t)


The Attempt at a Solution


First , 5=U_0, 314=\omega and voltage we can write as u=U_0cos(\omega t + \frac{\pi}{2}) and u=U_0 e^{i\frac{\pi}{2}}=iU_0. U is the voltage at the source U_1 in the branch and U_2 at the resistor. Now U=U_1+U_2 or U=IR+IZ where \frac{1}{Z}=\frac{1}{iL\omega}-\frac{C\omega}{i} or Z=\frac{iL\omega}{1-CL\omega^2}
Now the current is I=\frac{U}{R+Z} or when it is arranged I=\frac{iU_0(1-CL\omega^2)}{iL\omega (2-CL\omega^2)}. Now I don't know how to complete the calculation to reduce it to the form like this I_0sin(\omega t + \theta).
 

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If it is true that R = XL,XC, then XL = XC. What does that tell you about the LC tank circuit?
 
No just R=X_L.
 
masterjoda said:

Homework Statement


Find the current in them in this circuit, if we know R=X_L, X_C and u=5sin(314t)


The Attempt at a Solution


First , 5=U_0, 314=\omega and voltage we can write as u=U_0cos(\omega t + \frac{\pi}{2}) and u=U_0 e^{i\frac{\pi}{2}}=iU_0. U is the voltage at the source U_1 in the branch and U_2 at the resistor. Now U=U_1+U_2 or U=IR+IZ where \frac{1}{Z}=\frac{1}{iL\omega}-\frac{C\omega}{i} or Z=\frac{iL\omega}{1-CL\omega^2}
Now the current is I=\frac{U}{R+Z} or when it is arranged I=\frac{iU_0(1-CL\omega^2)}{iL\omega (2-CL\omega^2)}. Now I don't know how to complete the calculation to reduce it to the form like this I_0sin(\omega t + \theta).
Doesn't R=X_L, X_C, mean that R=X_L=X_C\ ?
 
masterjoda said:
No just R=X_L.

Ah, my bad. I read it as both being R, rather than as part of a list of known values. Where's a semicolon when you need one? :smile:

Anyways, you can write the complex impedances directly:

ZR = R

ZL = 0 + jR

ZC = 0 - jXC

These can then be used in formulas in the usual way to find voltages and currents (complex). Convert the values to phasor form at the end.
 
gneill said:
These can then be used in formulas in the usual way to find voltages and currents (complex). Convert the values to phasor form at the end.

I have used them and I got that last equation for I.
 
I'm not sure why you've gone to the "raw" L and C versions of the impedances when you've been given XL and XC. You should be able to find the total current as a complex function of u, R, and XC.
 
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