Is it possible to solve for VL in this parallel RL circuit?

In summary, the switch in the circuit will close and the circuit will be connected at time zero. However, it is not possible to calculate VL(t) as the resistor will be shorted. Without an additional inductor or resistor, it is not possible to maintain the voltage across the inductor.
  • #1
bphysics
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Homework Statement


I have the following parallel RC circuit. At time T = 0, the switch will close and the circuit will be connected. We assume that prior to T = 0, the circuit was at a steady-state.

p4CGr.png


I want to calculate VL(t) -- but I am being told that this is not possible for this problem, and would only be possible if there was an additional resistor or inductor (located where the switch is right now).

The professor and other individual who have told me this say that without this additional inductor / resistor, it is not possible to calculate VL(t) as the resistor will be shorted. This makes sense at T = 0, when the inductor will act as a short circuit, and the resistor will in-effect be shorted (as VL(0) = 0).. However, as T increases, the inductor will charge, and the voltage across the inductor will increase, until it acts as an open circuit and all current flows through R.

Therefore, I do not understand why it is not possible to solve for VL(t).

Can anyone provide clarification? I think this might just be miscommunication.

Homework Equations



The Attempt at a Solution

 
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  • #2
You are confusing inductor with capacitor. A capacitor will charge as T increases, which will eventually act as an open circuit.

On the other hand, an inductor will eventually act like a short circuit (after ~5 time constants).
 
  • #3
If Vs is an ideal voltage source then it will produce ANY amount of current necessary to maintain its voltage. When the switch closes, node A MUST therefore become equal to Vs, and must remain equal to Vs so long as the switch remains closed.

Normally the voltage across an inductor will go to zero as a circuit heads to steady state, with other circuit components like resistors or capacitors taking up the potential drop. Here it cannot, as Vs wants to maintain the potential and there's nowhere else for a drop to occur. The current through the inductor must therefore head off to infinity to satisfy the equation Vs = L di/dt.

For real components, current will be limited by non-ideal factors like internal resistance, stray inductance, stray capacitance, dielectric breakdown, etc. Something will probably go *BANG* :smile:
 
  • #4
You can certainly write the equation as gneill suggests.

The circuit is actually close to a real world circuit called a "buck-booster" used to step up or down a DC voltage. The inductor is initially connected to the voltage source on the left and the current allowed to build up in the inductor. When that current reaches a suitable level the inductor is disconnected from the voltage source and connected to the load on the right hand side where it dumps the energy stored in it.

Drawing:
http://www.mathworks.com/matlabcentral/fx_files/18833/3/content/html/buck_boost.png

Explanation:
http://www.mathworks.com/matlabcent...rol/content/html/ConfigurableDCConverter.html
 
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  • #5


As a scientist, it is important to approach problems with an open mind and consider all possibilities. In this case, it is possible that there may be a miscommunication between yourself and your professor/others. It is also possible that there may be some underlying assumptions or simplifications being made in the problem that are not explicitly stated.

In order to solve for VL(t), it is important to first understand the behavior of the circuit. As you mentioned, at T = 0, the inductor will act as a short circuit and the resistor will be shorted. This means that at this initial moment, the voltage across the inductor will be 0 and all current will flow through the resistor.

As time increases, the inductor will begin to charge and the voltage across it will also increase. However, this does not necessarily mean that all current will flow through the resistor. The inductor will still have a resistance, and as it charges, the voltage across it will reach a maximum and then start to decrease.

At this point, the voltage across the inductor may still be higher than the voltage across the resistor, meaning that some current will still flow through the inductor. It is only when the inductor reaches its maximum charge and the voltage across it drops to 0, that all current will flow through the resistor.

Therefore, it is possible to solve for VL(t) in this parallel RL circuit, but it may require some additional calculations and consideration of the behavior of the circuit over time. It is important to clarify with your professor/others what exactly they mean by "not possible to solve for VL(t)" and to discuss any underlying assumptions or simplifications being made in the problem.
 

1. What is a parallel RL circuit?

A parallel RL circuit is an electrical circuit that contains both a resistor (R) and an inductor (L) connected in parallel. This means that the components are connected to the same two points, and the current is split between them.

2. How do I calculate the total impedance in a parallel RL circuit?

To calculate the total impedance in a parallel RL circuit, you can use the formula Z = R + jXL, where Z is the total impedance, R is the resistance, and XL is the reactance of the inductor. This formula takes into account the resistive and reactive components of the circuit.

3. Is it possible to solve for VL in a parallel RL circuit?

Yes, it is possible to solve for VL in a parallel RL circuit. You can use the formula VL = IXL, where VL is the voltage across the inductor, I is the current, and XL is the reactance of the inductor. This formula takes into account the current and the reactance of the inductor.

4. Can I use Kirchhoff's voltage law to solve for VL in a parallel RL circuit?

Yes, you can use Kirchhoff's voltage law to solve for VL in a parallel RL circuit. Kirchhoff's voltage law states that the sum of the voltages around a closed loop in a circuit is equal to zero. By applying this law to the parallel RL circuit, you can solve for the voltage across the inductor.

5. What are the applications of a parallel RL circuit?

A parallel RL circuit has various applications, such as in power supplies, audio amplifiers, and filters. In power supplies, it is used to regulate voltage. In audio amplifiers, it is used to create a smooth and stable output signal. In filters, it is used to block certain frequencies and allow others to pass through.

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