202212201748 Solution to 2020-DSE-PHY-IA-23

Three identical resistors, a battery of negligible internal resistance, and an ideal voltmeter are connected to form Circuits (a) and (b) respectively.

Given that the voltmeter reading is 8\,\mathrm{V} in Circuit (a), what is the voltmeter reading in Circuit (b)?


Roughwork.

Redrawing a labelled diagram for (a),

and noting that

\begin{aligned} I_1=I_2 & = I/2 \\ I_3 & = 0 \\ I_4 & = I \\ R_\textrm{V}\parallel R & = R \\ R\parallel R & = R/2 \\ R_{\textrm{eq}} & = 3R/2 \\ \end{aligned}

we are about to write

\begin{aligned} I_4R & =8\,\mathrm{V}\textrm{ is given} \\ \mathcal{E} & =IR_{\textrm{eq}}\\ & = I\bigg(\frac{3R}{2}\bigg) \\ & = \frac{3}{2}(8) \\ & = 12\,\mathrm{V} \\ \end{aligned}

and obtain that the battery has an emf \mathcal{E} of 12\,\mathrm{V}. Likewise for (b),

where

\begin{aligned} I_2 & = I_4 \\ I_3 & = 0 \\ R_\textrm{V}\parallel R & = R \\ R+R_\textrm{V}\parallel R & = 2R \\ R\parallel (R+R_\textrm{V}\parallel R) & = 2R/3 \\ 12= \mathcal{E} & = I\bigg(\frac{2R}{3}\bigg) \\ \Longrightarrow\enspace IR & = 18 \\ \end{aligned}

\begin{aligned} & \quad\enspace \begin{cases} I_1R  =I_2(2R) \\ I_1+I_2 = 18/R \\ \end{cases} \\ & \Longrightarrow \begin{cases} I_1 = 12/R\\ I_2 = 6/R\\ \end{cases} \end{aligned}

being now asked for V=I_4R, the voltmeter reading, it is left to the reader.

202212071217 Solution to 1971-HL-PHY-I-7

The figure below shows a three-dimensional network in the form of a pyramid, in which A is the apex, and BCDE the square base.

Each of the eight edges of the pyramid is a wire of resistance 1\,\mathrm{\Omega}. A 12\,\mathrm{V} battery with internal resistance of 0.1\,\mathrm{\Omega} is connected across B and D. Calculate

(a) the power input of the network,
(b) the terminal voltage across the battery when current flows through the network, and
(c) the potential at the points B, C, D, and E if the apex A is earthed.


Roughwork.

Draw the circuit.

Label the potential.

Straighten the main.

Calculate the equivalent.

\begin{aligned} R_{\textrm{eq}} & = \big( R\parallel R\parallel R\big) + \big( R\parallel R\parallel R\big) \\ & = \frac{1}{\frac{1}{R}+\frac{1}{R}+\frac{1}{R}}\times 2 \\ & = \frac{2R}{3} \\ & = \frac{2(1)}{3} \\ & = \frac{2}{3}\,\mathrm{\Omega} \\ \end{aligned}

This problem is not to be attempted.

201902190827 Electric circuit diagrams (Elementary) Q13

The blogger claims no originality of his idea here.

We are given the following diagram:

Circuit0013

We would like to classify the nodes by the electric potential there. We label the nodes with a, b, c, etc. where the potential at a is larger than that at b, the potential at b is larger than that at c, etc. Therefore we have the following diagram:

Circuit0013Sol001

Aligning a, b, and c from left to right would give the main current direction. And we put each resistor back in between two consecutive nodes, (e.g., a and b, b and c, etc.) according to the two labels nearest to its two ends:

Circuit0013Sol002

And then the simplification is done.

201902190310 Electric circuit diagrams (Elementary) Q6

The blogger claims no originality of his question below.

Circuit0002

In the figure above, the resistors are identical. Find the equivalent resistance between nodes:

  1. a and b;
  2. c and d;
  3. b and c.

Solution.

  1. We label the nodes by A, B, C, etc. Different nodes with the same electric potential will be labelled with the same label, as shown below:
    Circuit0002Sol001
    Assuming resistors are identical, there is no current flowing through the central resistor between two equipotential end-nodes B‘s. Hence we draw the diagram below:
    Circuit0002Sol002
    The equivalent resistance is R_{\mathrm{eq}}=\displaystyle{\bigg( \frac{1}{R+R}+\frac{1}{R+R}\bigg)^{-1}}=R.(Alternatively one can use the Y\Delta transformation.)
  2. We draw the diagram below:
    Circuit0002Sol003
    The equivalent resistance between nodes c and d is given by \displaystyle{\frac{1}{R_{\mathrm{eq}}}}=\displaystyle{\frac{1}{R+R}}+\displaystyle{\frac{1}{R}}+\displaystyle{\frac{1}{R+R}}. Thus R_{\mathrm{eq}}=\displaystyle{\frac{R}{2}}.
  3. By Y\Delta transformation.