The home page presentation provides insight into the operation of two ideal LC circuits**:** A series-resonant circuit (without a series resistor), and a parallel-resonant circuit (without a parallel resistor). The author asserts that determining solution sets for ideal circuit configurations should precede attempts to analyze their parasitic-laden counterparts. Gaining an intuitive understanding of ideal circuit operation ought to be a high priority. Then, when parasitics are introduced, the practitioner will be better prepared to understand what is observed and, if necessary, synthesize what is needed for some particular application.

**Circuit 1** (a series-resonant configuration)**Initial Conditions**

1. The charge on the capacitor is 0. Therefore its voltage, V_{C}, is 0V

2. No current is flowing in the loop, nor is the current changing.**The Circuit Elements**

• The battery is ideal (no resistance, no inductance, and the voltage is invariant with load)

• The switch is ideal (**∞** Ohms when open, 0 Ohms when closed, no inductance, no bounce)

• The inductor is ideal (no resistance, no capacitance, and L is a fixed value)

• The capacitor is ideal (no resistance, no inductance, and C is a fixed value)

• The diode is ideal (no forward voltage drop, infinite reverse breakdown)

• The wire is ideal (no resistance, no inductance)**The Event**

At t=0 the switch closes, and remains closed**The Tasks**

1. Determine an expression for current in the loop.

2. Determine an expression for voltage on the inductor.

3. Determine an expression for voltage on the capacitor.**Observations**

• ..No current will be flowing just after the switch is thrown because current cannot change instantaneously in an inductor.

• The voltage will be 0V on the capacitor just after the switch is thrown because current has not begun flowing.

• Therefore all the battery voltage will appear across L just after the switch is thrown.

• The slope of V_{C} just after the switch is thrown must be zero because i=C(dv/dt), and i=0.

**Note**

Readers familiar with switching regulators should recognize**Figure 1** as an idealized building block. The diode is placed

to manage the current flowing in the inductor when the switch

opens (because the current cannot change instantaneously in

an inductor). In addition, there would exist some feedback

mechanism to control the switch in response to demands

placed on the load. Highly efficient regulators would specify

particular diode types, or they may even replace the diode

with some synchronized switch circuitry. The form this

synchronizing circuitry might take is not a subject of this work,

nor is the type of diode, nor the switch structure.

**The Analytic Solution**

If we write an equation for the voltage around the loop after the switch has closed, we get

**…….**V_{Batt} – L(di/dt) – (1/C)**∫**idt = 0

Or, using an abbreviated notation, we have

**…………**V_{Batt} – Li**‘** – (1/C)**∫**idt = 0

If we differentiate with respect to time, we see the following

**………………..**0 – Li**”** – i/C = 0

Multiplying by -1, and dividing by L yields a classic 2nd-order differential equation**………………….**i**”** + i/(LC) = 0

The general solution is given by**……………………………**i = Asinωt + Bcosωt

Where

**……………………………**ω = 1/SQRT(LC)

and where we note that

**……………………………**ω = 2πf

At time t=0 i is 0. Therefore, since sin0=0 and cos0=1, B must be 0, and we can write**……………………………**i = Asinωt

We note that

**…………………………..**v_{L} = Ldi/dt

Then

**…………………………..**v_{L} = LAωcosωt

At t=0 V_{L} equals V_{Batt}. The cosine of 0 is 1. So, we have**…………………………**V_{Batt} = LAω

Solving for A, we get

**……………………………**A = V_{Batt}/(Lω)

Substituting 1/SQRT(LC) for ω permits A to be written even more precisely as**……………………………**A = V_{Batt}(SQRT(C/L))

which is the peak current. The complete expression for i is then given by**……………………………**i = V_{Batt}(SQRT(C/L))sinωt

The peak current occurs when sinωt is 1. This occurs many times (because the circuit is oscillating). The first time it occurs is when ωt equals π/2. Solving for t, we have the following expression for the time of the first peak current**……………………………**t = π/2ω

Recalling that ω = 1/SQRT(LC), we can re-write the above equation, to give**……………………………**t = π(SQRT(LC))/2

which is the *first* occurrence of the peak current.

The voltage on the inductor is given by Ldi/dt. Thus (with a modicum of algebraic manipulation), we arrive at**…………………………..**v_{L} = LV_{Batt}(SQRT(C/L))ωcosωt

Then, substituting 1/SQRT(LC) for ω results in the following compact expression**…………………………..**v_{L} = V_{Batt}cosωt

Now, what about the peak voltage on the capacitor? Well,**…………………………..**v_{C} = (1/C)**∫**idt

Doing the integration produces the following result:**…………………………..**v_{C} = V_{Batt}(1/C)(SQRT(C/L))((-1/ω)cosωt + k)

Where k is a constant of integration. We have established that v_{C}=0 at t=0. Observing that cos0=1 leads us to the conclusion that k must be given by**……………………………**k = 1/ω

Gathering and re-arranging terms allow us to write**…………………………..**v_{C} = V_{Batt}(1/C)(SQRT(C/L))(1/ω)(1-cosωt)

But ω=1/SQRT(LC). Substituting this in, and then grinding through the math, gives the following succinct relationship**…………………………..**v_{C} = V_{Batt}(1-cosωt)

An easier way to get this solution would be to apply Kirkhoff’s voltage law on the loop, as follows:**…………………………..**v_{C} = V_{Batt} – v_{L}

Knowing that v_{L}=V_{Batt}cosωt leads to an identical expression for v_{C} (as it should).

cosωt ranges from +1 to -1. Therefore v_{C} ranges from 0 to 2V_{Batt} (indicating that this circuit is a voltage doubler). And when does it peak at 2V_{Batt}? That occurs whenever cosωt=-1, which occurs many times (because, again, this circuit is oscillating). But the first time it occurs is when the following relationship is satisfied**…………………………..**ωt = π

Solving for t, we get**……………………………**t = π/ω

which is twice the time it takes for the current to peak. Thus**……………………………**t = π(SQRT(LC))

which is the first occurrence of peak voltage on the capacitor.**Solution Summary for the Case of Zero-volt and Zero-current Initial Conditions**

**…………………………**i

_{Loop}= V

_{Batt}(SQRT(C/L))sinωt

**…………………………..**v

_{L}= V

_{Batt}cosωt

**…………………………..**v

_{C}= V

_{Batt}(1-cosωt)

where**……………………………**ω = 1/SQRT(LC)**Implications for Step-down Switching Regulators**

Ordinarily, the switch is opening & closing (regulating the output voltage to some level well below V

_{Batt}). But suppose (because of some circuit failure) it initially closes, and then does not re-open. The output will rise to twice the battery voltage. This could be catastrophic for the load, and must therefore be mitigated.

**A Note About Series Resistance**

With the possible exception of circuit operation near Absolute Zero (0°K), there are no known zero-resistance circuits. The switch (usually a MOSFET) and the inductor would be likely candidates for introducing enough series resistance to merit some investigation. It should be apparent that adding a series resistance will introduce an additional term in the loop equation. Interested readers are referred to

**Series RLC Circuitry**for analytical treatment of this condition.

**The More General**

**Case**

Although closing the switch when v

_{C}=0, and when i

_{Loop}=0 is an important case (i.e., a start-up for a switching regulator), two (likely simultaneous) initial conditions should also be considered. Those initial conditions are:

- A pre-existing loop current, I
_{0}(flowing in L, C, and through the diode)

- A pre-existing loop current, I

- A pre-existing voltage on the capacitor, V
_{C0}

- A pre-existing voltage on the capacitor, V

Recall that a regulated system has the switch opening & closing. We now define t=0 to be the moment just after the n^{th} closure of the switch. We assume again that some anomalous condition removes the switch from its usual controlled state of operation. That is, once closed it cannot re-open. Then we look again at Figure 1. We notice first that the diode is removed from consideration just as soon as it is forced to be in parallel with the battery. Current in the inductor cannot change instantaneously; therefore I_{0} continues to flow in L & C, but is diverted entirely to the battery. If we follow the original analysis it becomes apparent that we should now step in where, as before,**……………………………**i = Asinωt + Bcosωt

If we set t equal to 0 it becomes apparent that B=I_{0} (because the sine of 0 is 0, and the cosine of 0 is 1)

We note (again) that**…………………………..**v_{L} = Ldi/dt

Then**…………………………..**v_{L} = LAωcosωt – Bωsinωt

Noting that v_{C}(t=0) equals V_{C0 }(the defined initial condition), we can write

**………………………**v_{L}(t=0) = V_{Batt}-V_{C0}

And, because the cosine of 0 is 1, and the sine of 0 is 0, we can write**………………………**V_{Batt}-V_{C0} = LAω

A is now perfectly defined.**……………………………**A = (V_{Batt}-V_{C0})/Lω

Substituting 1/SQRT(LC) for ω permits A to be written even more precisely as**……………………………**A = (V_{Batt}-V_{C0})(SQRT(C/L))

So, we now have a complete solution for i using only the applied voltage, circuit values, and the given initial conditions.**……………………………**i = (V_{Batt}-V_{C0})(SQRT(C/L))sinωt + I_{0}cosωt

As before, the voltage on the inductor is given by Ldi/dt. So, we can write**…………………………..**v_{L} = L((V_{Batt}-V_{C0})(SQRT(C/L))ωcosωt – I_{0}ωsinωt)

Expanding ω to 1/SQRT(LC), we can simplify v_{L} to the following form**…………………………..**v_{L} = (V_{Batt}-V_{C0})cosωt – I_{0}SQRT(L/C)sinωt

At this point we express v_{C} as the battery voltage less the inductor voltage, as follows**…………………………..**v_{C} = V_{Batt} – (V_{Batt}-V_{C0})cosωt + I_{0}SQRT(L/C)sinωt

Rearranging gives**…………………………..**v_{C} = V_{Batt}(1-cosωt) + V_{C0}cosωt + I_{0}SQRT(L/C)sinωt

If (as a sanity check) we set V_{C0} to 0 and I_{0} to 0 we get precisely the same expression for v_{C} that derives from the start-up case (as we should). So, we now have a general solution summary for all cases.**Solution Summary for the General Case of Non-zero Initial Conditions**

**…………………………**i

_{Loop}= (V

_{Batt}-V

_{C0})(SQRT(C/L))sinωt + I

_{0}cosωt

**…………………………..**v

_{L}= (V

_{Batt}-V

_{C0})cosωt – I

_{0}SQRT(L/C)sinωt

**…………………………..**v

_{C}= V

_{Batt}(1-cosωt) + V

_{C0}cosωt + I

_{0}SQRT(L/C)sinωt

where**……………………………**ω = 1/SQRT(LC)**Circuit 2** (a parallel-resonant configuration)

Three ideal circuit elements in parallel**:**

- A current source (i
_{Source }= 0 for all t < 0, i_{Source}= I for all t > 0)

- An inductor, L

- A capacitor, C

**Initial Conditions**

The charge on the capacitor is 0. Therefore its voltage, V

_{C}, is 0V

No current is flowing anywhere in the network, nor is any current changing

**The Circuit Elements**

The current source is ideal (infinite impedance, no capacitance, and the current is invariant with voltage)

The inductor is ideal (no resistance, no capacitance, and L is a fixed value)

The capacitor is ideal (no resistance, no inductance, and C is a fixed value)

The wire is ideal (no resistance)

**The Event**

At t=0 the current source switches from 0A to I.

**The Tasks**

Determine an expression for the voltage across the network.

Determine an expression for current in the capacitor.

Determine an expression for current in the inductor.

**Observations**

The voltage will be 0V just after the current steps to I because voltage cannot change instantaneously on a capacitor.

i

_{L}= 0 just after the current steps to I because current cannot change instantaneously in an inductor.

i

_{C}= I just after the current steps to I because no current is flowing in the inductor.

Even though the

*magnitude*of V

_{C}at t=0 is 0V, the

*slope*of V

_{C }at t=0 must be >0 because i

_{C}=C(dv/dt), and i is I.

**The Analytic Solution**

Kirkhoff’s current law must be satisfied (the sum of the currents into any node must be zero). Thus,

**…………………..**I – i

_{L}– i

_{C}= 0

Recognizing that i

_{C}=Cdv/dt, and then re-writing, we get

**……………….**I – i

_{L}– Cdv/dt = 0

Differentiating with respect to time, we have

**……………..**0 – di

_{L}/dt – Cv

**”**= 0

But Ldi

_{L}/dt is the voltage on the inductor, which is the same as the voltage on the capacitor, which is v. So, we can write

**………………..**0 – v/L – Cv

**”**= 0

Multiplying through by -1, dividing by C, and then rearranging, gives

**………………….**v

**”**+ v/(LC) = 0

In form, this is identical to the switched-voltage case. Therefore, the solutions for v, i

_{C}, and i

_{L}will be sinusoidal, and the analysis proceeds in a manner similar to the series-resonant case. Without going through it step-by-step, the solution summary is given below.

**Solution Summary for the Case of Zero-volt and Zero-current Initial Conditions**

**……………**v

_{CurrentSource}= v

_{L}= v

_{C}= I(SQRT(L/C))sinωt

**…………………………..**i

_{C}= Icosωt

**…………………………..**i

_{L}= I(1-cosωt)

where

**……………………………**ω = 1/SQRT(LC)**Implications**

The current peak will be 2I in the inductor. This circuit may therefore be referred to as a current doubler. For that to predictably occur the current source must not saturate (if structured from a bipolar device) or go into the linear region of operation (if structured from a MOSFET). Therefore the peak voltage must be controlled by managing I, L, and C.**A Note About Parallel Resistance**With the possible exception of circuit operation near Absolute Zero (0°K), there are no known zero-resistance circuits. It should be apparent that adding a parallel resistance will introduce an additional term in the Kirkhoff equation. Interested readers are referred to

**Parallel RLC Circuitry**for an analytical treatment of this condition.

**What if the Input Source Does Not Differentiate to 0?**It may be that the input source is not a simple voltage or current step (each of which nicely differentiates to 0 for t>0). If that is the case, an appeal to one of the

**References**will lead to the concept of the “particular” integral (solution). Or, applying an online search engine to one of the following strings may lead an investigator to a circuit with the input source of interest.

• LC Circuits

• RLC Circuits