Understanding RLC Circuits: Series vs Parallel

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SUMMARY

This discussion focuses on the behavior of RLC circuits, specifically comparing series and parallel configurations. In a series RLC circuit, the inductor current is expressed as IL = IL, max * cos(ωt), while in a parallel RLC circuit, it is IL = -IL, max * cos(ωt). The voltage across all components in a parallel circuit remains constant, leading to different relationships between voltage and current for resistors, inductors, and capacitors. Understanding the phase relationships and the mathematical relationships between voltage and current is crucial for analyzing reactive circuits.

PREREQUISITES
  • Basic understanding of RLC circuit components: Resistors, Inductors, Capacitors
  • Familiarity with sinusoidal waveforms and their mathematical representations
  • Knowledge of voltage-current relationships in reactive components
  • Ability to interpret and sketch circuit diagrams
NEXT STEPS
  • Study the mathematical relationships in RLC circuits using Kirchhoff's laws
  • Learn about phasor analysis in AC circuits
  • Explore the concept of impedance in RLC circuits
  • Investigate the effects of damping in RLC circuits
USEFUL FOR

Electrical engineering students, circuit designers, and anyone interested in understanding the dynamics of RLC circuits in both series and parallel configurations.

hidemi
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Homework Statement
In a parallel RLC circuit, where IR = IR, max sin(ωt), the current through the inductor, IL, is

A) IL = −IL, max sin(ωt)

B) IL = IL, max sin(ωt)

C) IL = −IL, max cos(ωt)

D) IL = IL, max cos(ωt)

E) IL = IL, max tan(ωt)
Relevant Equations
I = Imax * sin(wt)
I'm a bit confused with RLC circuit.
If in series, IL = IL, max * cos(wt)
If in parallel, IL = - IL, max * cos(wt)
Are these correct?
 
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In a parallel RLC the voltage across all of the components is the same. So the voltage across the inductor is the same as the resistor voltage, which is proportional to the resistor current. But V = L(di/dt) for the inductor, which means that when the voltage across it is > 0 the inductor current is increasing V > 0, so di/di > 0. We also know that all of the voltages and currents are sinusoidal waves (assuming no non-sinusoidal driving source). So you can sketch the resistor current and use these rules to infer what the resulting inductor current will be.
 
DaveE said:
In a parallel RLC the voltage across all of the components is the same. So the voltage across the inductor is the same as the resistor voltage, which is proportional to the resistor current. But V = L(di/dt) for the inductor, which means that when the voltage across it is > 0 the inductor current is increasing V > 0, so di/di > 0. We also know that all of the voltages and currents are sinusoidal waves (assuming no non-sinusoidal driving source). So you can sketch the resistor current and use these rules to infer what the resulting inductor current will be.
Thanks for replying.
I wonder why there's a negative sign needed in front of IL ( IL = −IL, max cos(ωt) ).
Comparing to the following question, there is no negative sign needed in front of Ic. Why?

Q2:
In a parallel RLC circuit, where IR = IR, max sin(ωt), the current through the capacitor, Ic, is

The answer is: Ic = Ic, max cos(ωt)
 
hidemi said:
Thanks for replying.
I wonder why there's a negative sign needed in front of IL ( IL = −IL, max cos(ωt) ).
Comparing to the following question, there is no negative sign needed in front of Ic. Why?

Q2:
In a parallel RLC circuit, where IR = IR, max sin(ωt), the current through the capacitor, Ic, is

The answer is: Ic = Ic, max cos(ωt)
The difference lies in the relationship between the voltage and the current for each of those components.

Resistors: v = R⋅i, or i = v/R
Inductors: v = L⋅(di/dt), or i = (1/L)⋅∫v⋅dt
Capacitors: v = (1/C)⋅∫i⋅dt, or i = C⋅(dv/dt)

Notice the symmetry (or duality) between capacitors and inductors. The equations are essentially the same if you interchange voltage and current. There are many ways to describe this, but I think the best is for you to just graph the voltage ( v = R⋅i ), which is equal for all of the components in the parallel circuit. Then sketch in what the other curves must look like, since you know what dv/dt and ∫v⋅dt will look like. If you are more comfortable with one for vs. the other, you could work this backwards, where you sketch one of the currents and then figure out what the corresponding voltage must be.

The more analytical (mathematical) approach is to recall the derivatives and integrals for the sinusoids:
(d/dt)sin(t) = cos(t), (d/dt)cos(t) = -sin(t), ∫sin(t)⋅dt = -cos(t), ∫cos(t)⋅dt = sin(t); [ignoring integration constants]

This sort of understanding of the v - i relationship in these different components is key. It is the only way to really understand reactive circuits.
 
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As attached, I replaced the symbols of y axes that was used to represent RLC circuit in series, and now the graphs are for RLC circuit in parallel. I'd like to make sure I understand what you stated. thanks.
 

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hidemi said:
As attached, I replaced the symbols of y axes that was used to represent RLC circuit in series, and now the graphs are for RLC circuit in parallel. I'd like to make sure I understand what you stated. thanks.
I think it's OK. But there's no real way for me to say for sure, since you never defined what those variables are. In particular polarity. Is your inductor current pointing up, down, left, right? Plus I have absolutely no idea what ΔIL is. If you are going to show mathematically functions to describe circuit parameters, you must clearly define what those labels mean, or nobody will know what you are talking about. Circuit questions should always include a schematic diagram with variables labeled (particularly polarities).

Also, you include a 4th current ΔIL, which appears to have a small phase shift from the 0, π/2, π, -π/2 values. I don't understand how this applies to a parallel RLC circuit. You need to explain your problem as well as your answer. Otherwise we will assume it's the normal, most common, form, which, in this case, has no ΔIL (as I would define it).
 
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DaveE said:
I think it's OK. But there's no real way for me to say for sure, since you never defined what those variables are. In particular polarity. Is your inductor current pointing up, down, left, right? Plus I have absolutely no idea what ΔIL is. If you are going to show mathematically functions to describe circuit parameters, you must clearly define what those labels mean, or nobody will know what you are talking about. Circuit questions should always include a schematic diagram with variables labeled (particularly polarities).

Also, you include a 4th current ΔIL, which appears to have a small phase shift from the 0, π/2, π, -π/2 values. I don't understand how this applies to a parallel RLC circuit. You need to explain your problem as well as your answer. Otherwise we will assume it's the normal, most common, form, which, in this case, has no ΔIL (as I would define it).
Thank you! I think i have a better understanding of it based upon your comments and guiding questions.
 
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