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Question: Find equivalent Resistance blw A and B. $R_{AB}$=$R_{eq}$ = ? A R c R/2 R/4 R/8 R/16 R/32 R/64 R/1...

Find equivalent Resistance blw A and B.

RABR_{AB}=ReqR_{eq} = ?

A R c R/2 R/4 R/8 R/16 R/32 R/64 R/128

B R D R/2 R/4 R/8 R/16 R32\frac{R}{32} R/64 R128\frac{R}{128} \infty/ladder

Answer

R(1+172)R \left( \frac{1 + \sqrt{17}}{2} \right)

Explanation

Solution

The problem describes an infinite ladder network where the resistances in each subsequent section are scaled by a factor of 1/2. Let the equivalent resistance between points A and B be ReqR_{eq}.

The first "unit" of the ladder consists of:

  1. A resistor of value R in the upper branch (between A and C). Let's call this RACR_{AC}.
  2. A resistor of value R in the lower branch (between B and D). Let's call this RBDR_{BD}.
  3. A vertical resistor of value R connecting the upper and lower branches (between C and D). Let's call this RCD1R_{CD1}.

The network to the right of points C and D is an infinite ladder. All the resistances in this part of the network are half of the corresponding resistances in the original ladder. For example, the next horizontal resistors are R/2, the next vertical resistor is R/2, and so on. Therefore, if the equivalent resistance of the entire ladder from A to B is ReqR_{eq}, then the equivalent resistance of the infinite ladder starting from C and D will be Req/2R_{eq}/2. Let's call this RCD_ladderR_{CD\_ladder}.

Now, we can redraw the circuit by replacing the infinite ladder to the right of C and D with its equivalent resistance RCD_ladder=Req/2R_{CD\_ladder} = R_{eq}/2.

The circuit between points C and D now has two resistors in parallel:

  1. The vertical resistor RCD1=RR_{CD1} = R.
  2. The equivalent resistance of the rest of the ladder RCD_ladder=Req/2R_{CD\_ladder} = R_{eq}/2.

The equivalent resistance between C and D, due to these parallel components, is: RCD_parallel=RCD1RCD_ladderR_{CD\_parallel} = R_{CD1} \parallel R_{CD\_ladder} RCD_parallel=R×(Req/2)R+(Req/2)R_{CD\_parallel} = \frac{R \times (R_{eq}/2)}{R + (R_{eq}/2)} RCD_parallel=RReq2R+ReqR_{CD\_parallel} = \frac{R \cdot R_{eq}}{2R + R_{eq}}

Now, the entire circuit from A to B can be viewed as three resistors in series:

  1. RACR_{AC} (from A to C)
  2. RCD_parallelR_{CD\_parallel} (from C to D)
  3. RBDR_{BD} (from D to B)

So, the equivalent resistance ReqR_{eq} is: Req=RAC+RCD_parallel+RBDR_{eq} = R_{AC} + R_{CD\_parallel} + R_{BD} Substitute the values: RAC=RR_{AC} = R, RBD=RR_{BD} = R. Req=R+RReq2R+Req+RR_{eq} = R + \frac{R \cdot R_{eq}}{2R + R_{eq}} + R Req=2R+RReq2R+ReqR_{eq} = 2R + \frac{R \cdot R_{eq}}{2R + R_{eq}}

Now, we solve this equation for ReqR_{eq}. Let X=ReqX = R_{eq}. X=2R+RX2R+XX = 2R + \frac{RX}{2R + X} Multiply both sides by (2R+X)(2R + X): X(2R+X)=2R(2R+X)+RXX(2R + X) = 2R(2R + X) + RX 2RX+X2=4R2+2RX+RX2RX + X^2 = 4R^2 + 2RX + RX 2RX+X2=4R2+3RX2RX + X^2 = 4R^2 + 3RX Rearrange the terms to form a quadratic equation: X2RX4R2=0X^2 - RX - 4R^2 = 0

Using the quadratic formula X=b±b24ac2aX = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}, where a=1a=1, b=Rb=-R, c=4R2c=-4R^2: X=(R)±(R)24(1)(4R2)2(1)X = \frac{-(-R) \pm \sqrt{(-R)^2 - 4(1)(-4R^2)}}{2(1)} X=R±R2+16R22X = \frac{R \pm \sqrt{R^2 + 16R^2}}{2} X=R±17R22X = \frac{R \pm \sqrt{17R^2}}{2} X=R±R172X = \frac{R \pm R\sqrt{17}}{2} Since resistance must be a positive value, we take the positive root: Req=R+R172R_{eq} = \frac{R + R\sqrt{17}}{2} Req=R(1+172)R_{eq} = R \left( \frac{1 + \sqrt{17}}{2} \right)

The final answer is R(1+172)R \left( \frac{1 + \sqrt{17}}{2} \right).

Explanation of the solution:

  1. Identify the repeating pattern: The network is an infinite ladder where each subsequent section's resistances are scaled by 1/2.
  2. Define equivalent resistance: Let the equivalent resistance of the entire infinite ladder be ReqR_{eq}.
  3. Utilize infinite ladder property: Due to the scaling, the equivalent resistance of the ladder starting from the second set of nodes (C and D) is Req/2R_{eq}/2.
  4. Simplify the first section: The vertical resistor (R) in the first section is in parallel with the equivalent resistance of the rest of the ladder (Req/2R_{eq}/2). Calculate this parallel combination.
  5. Formulate the equation: The two horizontal resistors (R each) in the first section are in series with the calculated parallel combination. Set up an equation for ReqR_{eq}.
  6. Solve the quadratic equation: Solve the resulting quadratic equation for ReqR_{eq}, choosing the positive root as resistance cannot be negative.