Ph · Physics

How to Calculate the Equivalent Capacitance of an Infinite Ladder

Published By the 9to5Science editorial team

At a glance

  1. 1. Identify the repeating cell

    Assume each ladder section contains one series capacitor and one identical capacitor connected to ground.

  2. 2. Use self-similarity

    The entire infinite ladder beyond the first series capacitor has the same equivalent capacitance as the full ladder.

  3. 3. Combine the capacitors

    The shunt capacitor is in parallel with the remaining ladder, and that combination is in series with the first capacitor.

  4. 4. Solve the quadratic

    Choose the positive physical solution for the equivalent capacitance.

An “infinite ladder of capacitors” is not completely defined without a circuit diagram. The standard interpretation is a repeating network of identical capacitors: one capacitor in series along the top branch, followed at each node by one capacitor connected to ground. The input terminals are the leftmost top node and ground.

For that topology, the infinite ladder has a finite equivalent capacitance:

Ceq=5−12C≈0.618C.C_{\mathrm{eq}}=\frac{\sqrt{5}-1}{2}C\approx 0.618C.

The result is smaller than one capacitor CC because the first capacitor is in series with the rest of the network.

The standard ladder topology

Label the capacitance of every capacitor by CC. Starting at the input, the circuit consists of:

  1. A series capacitor CC.
  2. A node connected to ground through a capacitor CC.
  3. The same pattern repeated indefinitely to the right.

Let XX denote the equivalent capacitance seen at the input terminals. Because the ladder is infinite and every section is identical, removing the first section leaves a network whose equivalent capacitance is also XX.

This self-similarity is the key idea.

Set up the equivalent-capacitance equation

After the first series capacitor, the next node sees two branches to ground:

  • the vertical capacitor, with capacitance CC;
  • the remaining infinite ladder, with equivalent capacitance XX.

These two branches are in parallel, so their combined capacitance is

C∥=C+X.C_{\parallel}=C+X.

That parallel combination is in series with the first capacitor CC. The equivalent capacitance of two capacitors in series is

Cseries=C1C2C1+C2.C_{\mathrm{series}}=\frac{C_1C_2}{C_1+C_2}.

Therefore,

X=C(C+X)C+(C+X)=C(C+X)2C+X.X=\frac{C(C+X)}{C+(C+X)} =\frac{C(C+X)}{2C+X}.

Solve the equation

Multiply both sides by 2C+X2C+X:

X(2C+X)=C(C+X).X(2C+X)=C(C+X).

Expand both sides:

2CX+X2=C2+CX.2CX+X^2=C^2+CX.

Rearrange into a quadratic equation:

X2+CX−C2=0.X^2+CX-C^2=0.

Using the quadratic formula,

X=−C±C2+4C22=−C±5C2.X=\frac{-C\pm\sqrt{C^2+4C^2}}{2} =\frac{-C\pm\sqrt{5}C}{2}.

Capacitance must be nonnegative, so discard the negative root. The physical solution is

Ceq=5−12C.\boxed{C_{\mathrm{eq}}=\frac{\sqrt{5}-1}{2}C}.

Since

5−12≈0.618034,\frac{\sqrt{5}-1}{2}\approx 0.618034,

the infinite ladder has an equivalent capacitance of about 61.8%61.8\% of the capacitance of one individual capacitor.

Numerical example

Suppose every capacitor has capacitance

C=10 nF.C=10\ \mathrm{nF}.

Then

Ceq=5−12(10 nF)≈6.18 nF.C_{\mathrm{eq}}=\frac{\sqrt{5}-1}{2}(10\ \mathrm{nF}) \approx 6.18\ \mathrm{nF}.

The first series capacitor alone would give an upper bound of 10 nF10\ \mathrm{nF}, because the rest of the ladder cannot make the series combination larger than either series component. The result 6.18 nF6.18\ \mathrm{nF} is consistent with that bound.

Why an infinite circuit can have a finite answer

“Infinite” refers to the number of components, not to an infinite capacitance. Each additional section is connected through more series capacitors, so its influence on the input becomes progressively limited.

One way to verify convergence is to calculate finite ladders. If XnX_n is the equivalent capacitance of a ladder with nn repeated sections, then

Xn+1=C(C+Xn)2C+Xn,X_{n+1}=\frac{C(C+X_n)}{2C+X_n},

with X1=C/2X_1=C/2 for one series capacitor followed by one shunt capacitor. The sequence approaches 0.618034C0.618034C as nn increases.

For example, in units where C=1C=1:

Number of sectionsEquivalent capacitance
10.5000.500
20.6000.600
30.6150.615
40.61760.6176
Infinite limit0.6180340.618034

The infinite result is the limit of increasingly long finite ladders.

Common mistakes

Treating every capacitor as parallel

Capacitors are parallel only when they connect between the same two nodes. The vertical capacitors do not all share the same upper node, so they cannot simply be added together.

Treating every capacitor as series

The ladder contains branching nodes. Once a vertical capacitor connects to ground, the circuit is no longer one single series chain.

Choosing the negative quadratic root

The other algebraic solution is

X=−1+52C,X=-\frac{1+\sqrt{5}}{2}C,

which is negative for positive CC. It does not represent the equivalent capacitance of ordinary passive capacitors.

Assuming every “infinite ladder” has this answer

The value depends on the topology and on the capacitances. If the series capacitors and shunt capacitors have different values, say CsC_s and CpC_p, then the same method gives

X=Cs(Cp+X)Cs+Cp+X.X=\frac{C_s(C_p+X)}{C_s+C_p+X}.

After rearranging,

X2+CpX−CsCp=0,X^2+C_pX-C_sC_p=0,

so the positive solution is

X=−Cp+Cp2+4CsCp2.X=\frac{-C_p+\sqrt{C_p^2+4C_sC_p}}{2}.

Other arrangements—such as a ladder with alternating series and parallel blocks, or capacitors connected between adjacent nodes without a ground rail—require a different equation. The circuit’s node connections must be specified before an equivalent capacitance can be calculated.

References

  1. Introduction to Electrodynamics, David J. Griffiths
  2. Fundamentals of Physics, Halliday, Resnick, and Walker

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