2020 A/L Physics Past Paper · Question 47 (English Medium)

An endless ladder network — the equivalent resistance between A and B

An endless ladder network made of 1 Ω1\ \Omega resistors is shown in the figure. If RR is the equivalent resistance of this network between the points AA and BB, which of the following is true?

  1. (1) R<2 ΩR < 2\ \Omega
  2. (2) R=2 ΩR = 2\ \Omega
  3. (3) R>3 ΩR > 3\ \Omega
  4. (4) R=3 ΩR = 3\ \Omega
  5. (5) 2 Ω<R<3 Ω2\ \Omega < R < 3\ \Omega
Answer and explanation

Answer: (5) 2 Ω<R<3 Ω2\ \Omega < R < 3\ \Omega

What the question asks

We must find: the range in which the equivalent resistance RR between AA and BB of the endless ladder lies.

Given information

Given: every resistor is 1 Ω1\ \Omega; each section has one on the top rail, one on the bottom rail, then a rung across; this pattern continues without end.

Relevant theory

V =IR, where R is a constant.

"The algebraic sum of the currents flowing across a junction of a circuit is zero".

Reasoning and calculation

Structure: from AA, a top 1 Ω1\ \Omega to junction CC; from BB, a bottom 1 Ω1\ \Omega to junction DD; between CC and DD, the first rung 1 Ω1\ \Omega; the rest of the ladder continues from the same CC, DD.

Symmetry (self-similarity): the ladder is endless; removing the first section leaves, from CC, DD, the exact same endless ladder. So the resistance of the remaining ladder between CC and DD is also RR.

Nodes: A→CA \to C on the top rail and D→BD \to B on the bottom rail carry the whole current (series). Between CC and DD there are two paths: the rung 1 Ω1\ \Omega and the rest of the ladder RR — the same potential difference across both.

Reducing: replacing the rest of the ladder by one resistance RR, the network becomes 1 Ω1\ \Omega — (1 Ω∥R1\ \Omega \parallel R) — 1 Ω1\ \Omega in series. By Kirchhoff's first law at junction CC, I=VCD1+VCDRI = \dfrac{V_{CD}}{1} + \dfrac{V_{CD}}{R}; so the equivalent resistance between CC and DD is VCDI=R1+R\dfrac{V_{CD}}{I} = \dfrac{R}{1 + R}.

Required equations

Rseries=R1+R2+⋯R_{\text{series}} = R_1 + R_2 + \cdots

I=VR1+VR2  ⇒  R∥=R1R2R1+R2I = \frac{V}{R_1} + \frac{V}{R_2} \;\Rightarrow\; R_{\parallel} = \frac{R_1R_2}{R_1 + R_2}

R=1+1×R1+R+1R = 1 + \frac{1 \times R}{1 + R} + 1

R(1+R)=2(1+R)+R  ⇒  R2−2R−2=0R(1 + R) = 2(1 + R) + R \;\Rightarrow\; R^2 - 2R - 2 = 0

2.732.73

R=2+4+82=1+3R = \frac{2 + \sqrt{4 + 8}}{2} = 1 + \sqrt{3}

Physical root: the other root of R2−2R−2=0R^2 - 2R - 2 = 0 is 1−3<01 - \sqrt3 < 0 — a resistance cannot be negative; so R=1+3≈2.73 ΩR = 1 + \sqrt3 \approx 2.73\ \Omega, i.e. 2 Ω<R<3 Ω2\ \Omega < R < 3\ \Omega.

Reading the options

Comparing with the options: R≈2.73 ΩR \approx 2.73\ \Omega — option (5) 2 Ω<R<3 Ω2\ \Omega < R < 3\ \Omega.

Checks

1+sqrt(3)1 + sqrt(3)

Boundary check: a single section alone is 1+1+1=3 Ω1 + 1 + 1 = 3\ \Omega (the rest an open circuit — an upper bound); the rest as a short circuit gives 2 Ω2\ \Omega (a lower bound). The true RR lies between these. Second way (finite ladders): n=1n = 1: 33; n=2n = 2: 2+34=2.752 + \dfrac{3}{4} = 2.75; n=3n = 3: 2+2.753.75=2.7332 + \dfrac{2.75}{3.75} = 2.733 — converging toward 2.7322.732 ✓.

Conclusion

R=1+3≈2.73 ΩR = 1 + \sqrt{3} \approx 2.73\ \Omega

The rest of the ladder is also RR: R=2+R1+RR = 2 + \dfrac{R}{1 + R}, giving R=1+3≈2.73 ΩR = 1 + \sqrt3 \approx 2.73\ \Omega — the answer is (5) 2 Ω<R<3 Ω2\ \Omega < R < 3\ \Omega.

Assuming the resistance keeps increasing as more sections are added to the endless ladder.

Every new section joins in parallel with the previous rung: the resistance decreases and settles at 1+31 + \sqrt3.

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