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Question: Two circuits (as shown in the following figure) are called Circuit A and Circuit B. The equivalent r...

Two circuits (as shown in the following figure) are called Circuit A and Circuit B. The equivalent resistance of Circuit A is x and that of Circuit B is y (between 1 and 2). The value of yxy-x is ηR\eta R. Then the value of η\eta is _____.

Answer

0.0593

Explanation

Solution

To find the value of η\eta, we first need to calculate the equivalent resistances of Circuit A (xx) and Circuit B (yy). Both are infinite ladder networks, which can be solved by assuming the equivalent resistance of the infinite part of the circuit is the same as the total equivalent resistance.

Circuit A Analysis:

Circuit A is a ladder network where each repeating unit consists of a 2R2R resistor in the horizontal branch and an RR resistor in the vertical branch, connecting the top rail to the bottom rail.

Let xx be the equivalent resistance of Circuit A between terminals 1 and 2. If we consider the first unit cell (a 2R2R horizontal resistor and an RR vertical resistor), the rest of the infinite ladder network (from the node after the first 2R2R resistor to the bottom rail) will also have an equivalent resistance of xx.

The equivalent resistance xx can be expressed as: The 2R2R resistor is in series with the parallel combination of the vertical RR resistor and the equivalent resistance xx of the rest of the ladder. x=2R+RxR+xx = 2R + \frac{R \cdot x}{R + x} To solve for xx, multiply both sides by (R+x)(R+x): x(R+x)=2R(R+x)+Rxx(R+x) = 2R(R+x) + Rx Rx+x2=2R2+2Rx+RxRx + x^2 = 2R^2 + 2Rx + Rx Rx+x2=2R2+3RxRx + x^2 = 2R^2 + 3Rx Rearrange into a quadratic equation: x22Rx2R2=0x^2 - 2Rx - 2R^2 = 0 Using the quadratic formula x=b±b24ac2ax = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}, where a=1a=1, b=2Rb=-2R, c=2R2c=-2R^2: x=(2R)±(2R)24(1)(2R2)2(1)x = \frac{-(-2R) \pm \sqrt{(-2R)^2 - 4(1)(-2R^2)}}{2(1)} x=2R±4R2+8R22x = \frac{2R \pm \sqrt{4R^2 + 8R^2}}{2} x=2R±12R22x = \frac{2R \pm \sqrt{12R^2}}{2} x=2R±2R32x = \frac{2R \pm 2R\sqrt{3}}{2} Since resistance must be positive, we take the positive root: x=R(1+3)x = R(1 + \sqrt{3})

Circuit B Analysis:

Circuit B is a different type of ladder network. Each repeating unit consists of a 2R2R resistor in the top horizontal branch, an RR resistor in the bottom horizontal branch, and an RR resistor connecting the two horizontal branches.

Let yy be the equivalent resistance of Circuit B between terminals 1 and 2. If we consider the first unit cell (a 2R2R top horizontal, an RR vertical, and an RR bottom horizontal resistor), the rest of the infinite ladder network (from the nodes after this first unit) will also have an equivalent resistance of yy.

The equivalent resistance yy can be expressed as: The 2R2R resistor (top) is in series with a parallel combination. This parallel combination consists of the vertical RR resistor and the series combination of the bottom RR resistor and the equivalent resistance yy of the rest of the ladder. y=2R+R(R+y)R+(R+y)y = 2R + \frac{R \cdot (R+y)}{R + (R+y)} y=2R+R2+Ry2R+yy = 2R + \frac{R^2 + Ry}{2R + y} To solve for yy, multiply both sides by (2R+y)(2R+y): y(2R+y)=2R(2R+y)+R2+Ryy(2R+y) = 2R(2R+y) + R^2 + Ry 2Ry+y2=4R2+2Ry+R2+Ry2Ry + y^2 = 4R^2 + 2Ry + R^2 + Ry 2Ry+y2=5R2+3Ry2Ry + y^2 = 5R^2 + 3Ry Rearrange into a quadratic equation: y2Ry5R2=0y^2 - Ry - 5R^2 = 0 Using the quadratic formula y=b±b24ac2ay = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}, where a=1a=1, b=Rb=-R, c=5R2c=-5R^2: y=(R)±(R)24(1)(5R2)2(1)y = \frac{-(-R) \pm \sqrt{(-R)^2 - 4(1)(-5R^2)}}{2(1)} y=R±R2+20R22y = \frac{R \pm \sqrt{R^2 + 20R^2}}{2} y=R±21R22y = \frac{R \pm \sqrt{21R^2}}{2} y=R±R212y = \frac{R \pm R\sqrt{21}}{2} Since resistance must be positive, we take the positive root: y=R(1+21)2y = \frac{R(1 + \sqrt{21})}{2}

Calculate η\eta:

We are given that yx=ηRy-x = \eta R. yx=R(1+21)2R(1+3)y-x = \frac{R(1 + \sqrt{21})}{2} - R(1 + \sqrt{3}) Factor out RR: yx=R(1+212(1+3))y-x = R \left( \frac{1 + \sqrt{21}}{2} - (1 + \sqrt{3}) \right) yx=R(1+212(1+3)2)y-x = R \left( \frac{1 + \sqrt{21} - 2(1 + \sqrt{3})}{2} \right) yx=R(1+212232)y-x = R \left( \frac{1 + \sqrt{21} - 2 - 2\sqrt{3}}{2} \right) yx=R(212312)y-x = R \left( \frac{\sqrt{21} - 2\sqrt{3} - 1}{2} \right) Comparing this with yx=ηRy-x = \eta R, we get: η=212312\eta = \frac{\sqrt{21} - 2\sqrt{3} - 1}{2}

The value of 214.5826\sqrt{21} \approx 4.5826 and 31.732\sqrt{3} \approx 1.732. η=4.58262(1.732)12\eta = \frac{4.5826 - 2(1.732) - 1}{2} η=4.58263.46412\eta = \frac{4.5826 - 3.464 - 1}{2} η=0.11862\eta = \frac{0.1186}{2} η=0.0593\eta = 0.0593

The question asks for the value of η\eta.

The final answer is 0.0593\boxed{0.0593}.

Explanation of the solution:

  1. Identify the repeating unit: For both infinite ladder circuits, identify the basic repeating unit.
  2. Formulate the self-similarity equation: Assume the equivalent resistance of the infinite ladder is ReqR_{eq}. Replace the infinite part of the circuit after the first repeating unit with ReqR_{eq} itself.
  3. Solve the quadratic equation: The resistance equation will typically reduce to a quadratic equation. Solve for the positive root, as resistance cannot be negative.
  4. Calculate the difference: Subtract the equivalent resistance of Circuit A (xx) from that of Circuit B (yy) and express the result in the form ηR\eta R to find η\eta.

Answer: The value of η\eta is 212312\frac{\sqrt{21} - 2\sqrt{3} - 1}{2}. Numerically, η0.0593\eta \approx 0.0593.