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Question: A normal 8 × 8 chessboard is made from plates of two different metals, both of which are quite poor ...

A normal 8 × 8 chessboard is made from plates of two different metals, both of which are quite poor electrical conductors. The only other conducting elements in its construction are two thin terminal strips, which have very good conductivity. They are positioned one at each end of the board (but not shown in the figure). The common thickness t of the plates is much less than the length L of the board.

The conductivity of the light squares is σ1\sigma_1, and that of the dark ones is σ2\sigma_2. Find the current flowing through the chessboard, if a steady voltage V is applied across the terminals. Any interface resistances between the squares can be neglected.

Answer

V \frac{2t \sigma_1 \sigma_2}{\sigma_1 + \sigma_2}

Explanation

Solution

The problem describes an 8x8 chessboard made of two different metals with conductivities σ1\sigma_1 and σ2\sigma_2. A voltage V is applied across the ends of the board. The current flows along the length L of the board.

  1. Dimensions of a single square:

    The chessboard is 8x8, and its total length is L. Therefore, the side length of each individual square is s=L/8s = L/8. The thickness of the plates is given as tt.

  2. Resistance of a single square:

    The current flows along the length 's' of each square. The cross-sectional area perpendicular to the current flow for a single square is A=s×t=(L/8)tA = s \times t = (L/8)t. The resistance of a conductor is given by R=ρlengthareaR = \rho \frac{\text{length}}{\text{area}}, where ρ=1/σ\rho = 1/\sigma is the resistivity. For a light square (conductivity σ1\sigma_1): R1=1σ1ss×t=1σ1tR_1 = \frac{1}{\sigma_1} \frac{s}{s \times t} = \frac{1}{\sigma_1 t} For a dark square (conductivity σ2\sigma_2): R2=1σ2ss×t=1σ2tR_2 = \frac{1}{\sigma_2} \frac{s}{s \times t} = \frac{1}{\sigma_2 t}

  3. Resistance of a single row:

    A chessboard has alternating light and dark squares. In an 8x8 board, each row consists of 8 squares. Since they alternate, there will be 4 squares of type σ1\sigma_1 and 4 squares of type σ2\sigma_2 in each row. These squares are connected in series along the direction of current flow. The total resistance of one row (RrowR_{row}) is the sum of the resistances of these 8 squares: Rrow=4R1+4R2R_{row} = 4R_1 + 4R_2 Rrow=4(1σ1t)+4(1σ2t)R_{row} = 4 \left( \frac{1}{\sigma_1 t} \right) + 4 \left( \frac{1}{\sigma_2 t} \right) Rrow=4t(1σ1+1σ2)R_{row} = \frac{4}{t} \left( \frac{1}{\sigma_1} + \frac{1}{\sigma_2} \right) Rrow=4t(σ1+σ2σ1σ2)R_{row} = \frac{4}{t} \left( \frac{\sigma_1 + \sigma_2}{\sigma_1 \sigma_2} \right)

  4. Equivalent resistance of the chessboard:

    The 8 rows of the chessboard are connected in parallel across the voltage V. Since all rows are identical, the equivalent resistance (ReqR_{eq}) of the entire chessboard is: 1Req=1Rrow+1Rrow+(8 times)\frac{1}{R_{eq}} = \frac{1}{R_{row}} + \frac{1}{R_{row}} + \dots \text{(8 times)} 1Req=8Rrow\frac{1}{R_{eq}} = \frac{8}{R_{row}} Req=Rrow8R_{eq} = \frac{R_{row}}{8} Substitute the expression for RrowR_{row}: Req=18[4t(σ1+σ2σ1σ2)]R_{eq} = \frac{1}{8} \left[ \frac{4}{t} \left( \frac{\sigma_1 + \sigma_2}{\sigma_1 \sigma_2} \right) \right] Req=12t(σ1+σ2σ1σ2)R_{eq} = \frac{1}{2t} \left( \frac{\sigma_1 + \sigma_2}{\sigma_1 \sigma_2} \right)

  5. Current flowing through the chessboard:

    Using Ohm's Law, I=VReqI = \frac{V}{R_{eq}}: I=V12t(σ1+σ2σ1σ2)I = \frac{V}{\frac{1}{2t} \left( \frac{\sigma_1 + \sigma_2}{\sigma_1 \sigma_2} \right)} I=V2tσ1σ2σ1+σ2I = V \frac{2t \sigma_1 \sigma_2}{\sigma_1 + \sigma_2}

The current flowing through the chessboard is V2tσ1σ2σ1+σ2V \frac{2t \sigma_1 \sigma_2}{\sigma_1 + \sigma_2}.