Current through source in AC circuit with R & LC in parallel

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The discussion focuses on calculating the effective current through a source in an AC circuit with resistive and LC components in parallel. The impedance is determined using the formula Z = √(R² + (XL - Xc)²), leading to the conclusion that the total impedance can be calculated similarly to resistances in parallel. The participants confirm that the phasor diagram approach is valid and that the total impedance must account for the series combination of the inductor and capacitor. The correct method involves calculating the total impedance and then using it to find the RMS current through the circuit. The conversation emphasizes that while the initial answer was correct, the approach can be systematically verified through impedance calculations.
Shivang kohlii
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Homework Statement


In the circuit diagram shown , Xc = 100 ohm , XL = 200 ohm , R = 100 ohm , the effective current through the source is ?

Homework Equations


Z= √( R^2 + ( XL - Xc)^2)
Vrms = Irms/ Z

The Attempt at a Solution


I tried to draw the phaser diagram and calculate the relation between the current in the LC branch and current in R branch( the phaser diagram is given as attachment)
From it I concluded that Inet = √( (I1)^2 + (I2)^2)
Where I1 = current through R branch
I2 = current through LC branch
And I got ans= 2√2 which is correct
1.What I am confused is that was my answer just by chance
2.And is it even possible to draw phaser diagrams when in parallel.. if yes, then is my attempt correct ?
3.If not , how else can we solve it .. or is there any easier method to solve it?
 

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In relation to applied voltage, what is the phase angle of current thru a:
Resistor?
Capacitor?
Inductor?
 
I think your answer (and the associated reasoning) is correct but it can't be solved in a simpler way.

We know that when we have elements in parallel the total impedance is computed in a similar way like when we have resistances in parallel.

In this circuit it would be $$\frac{1}{Z}=\frac{1}{Z_R}+\frac{1}{Z_{L+C}} \text{(1)}$$ where ##Z## is the total impedance of the circuit and ##Z_{L+C}## is the total impedance of the branch that contains the L and C. Because L and C are in series it is ##Z_{L+C}=Z_L+Z_C=i{(X_L-X_C)}=i100 Ohm##

Also ##Z_R=R=100Ohm##

So by (1) you can calculate ##Z##, and then calculate ##I_{rms}=V_{rms}/|Z|##
 
Last edited:
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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