201902190842 Electric field representation

The blogger claims no originality of his question posted here.

Think of a field in some representation other than a diagram of field lines. For instance, suppose any point in a field is assigned a number to its field strength magnitude, but the direction of field strength of each point is not indicated. Now, could we deduce a rough picture of the (vector) E-field from these (scalar) numbers, provided that we know the distribution of these numbers and the position of charges?

Visualizing_the_Efield_by_numbers_distribution

In the figure, A, B and C are charges of unknown charge quantities and sign. Each single-digit number at a point represents the magnitude of E-field strength at that point. For example, 6 stands for 6\,\mathrm{N/C}, 0 stands for zero E-field, i.e., a neutral point. By deducing from the figure, determine which of the following statements is/are correct.

(1) Charge quantity of A is larger than that of either B or C.
(2) Charge quantity of B equals charge quantity of C.
(3) Charge A is positive. Charge B and charge C are both negative.

A. (1) only
B. (2) only
C. (1) and (2) only
D. (1), (2), and (3)


Answer. D

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.