A uniform wire of resistance 9Ω is bent in the form of an equilateral triangle. Find the effective resistance across a side of the triangle.
2 Ω
This problem asks us to find the effective resistance across one side of a uniform wire that has been bent into the shape of an equilateral triangle. The total resistance of the wire is given as 9 \(\Omega\).
When a uniform wire with total resistance \(R_{total}\) is bent into an equilateral triangle, the resistance is distributed equally along each side. Since an equilateral triangle has three equal sides, the resistance of each side will be one-third of the total resistance.
Let \(R_{side}\) be the resistance of one side of the triangle.
So, each side of the equilateral triangle has a resistance of 3 \(\Omega\).
To find the effective resistance across one side, let's consider finding the resistance across side AB of the triangle ABC. The current enters at point A and leaves at point B. The path through side AB is one direct path with resistance 3 \(\Omega\). The other path is through the remaining two sides, AC and CB, which are connected in series between points A and B.
The resistance of side AC is 3 \(\Omega\), and the resistance of side CB is also 3 \(\Omega\). When resistors are in series, their resistances add up.
Resistance of series path (AC + CB) = \(3 \Omega + 3 \Omega = 6 \Omega\).
Now we have two paths between points A and B:
These two paths are in parallel. The formula for the effective resistance (\(R_{eff}\)) of two resistors (\(R_1\) and \(R_2\)) in parallel is:
In this case, \(R_1 = 3 \Omega\) and \(R_2 = 6 \Omega\). Plugging these values into the formula:
The effective resistance across a side of the equilateral triangle is 2 \(\Omega\).
| Step | Description | Calculation | Result |
|---|---|---|---|
| 1 | Resistance per side | Total Resistance / 3 | |
| 2 | Resistance of series part (2 sides) | Resistance of side 1 + Resistance of side 2 | |
| 3 | Effective resistance (Parallel combination) | (Rparallel * Rseries) / (Rparallel + Rseries) |
| Concept | Description | Formula |
|---|---|---|
| Resistance of uniform wire segment | Proportional to length | \(R \propto L\) |
| Resistors in Series | Total resistance is the sum of individual resistances | |
| Resistors in Parallel | Reciprocal of total resistance is the sum of reciprocals of individual resistances |
Problems involving wires bent into shapes often require identifying series and parallel combinations. A uniform wire means resistance is directly proportional to length. When a wire is bent into a polygon, and the resistance is measured across one side (or between two vertices), the remaining parts of the wire form a network, typically involving series and parallel connections. For symmetrical shapes like equilateral triangles, squares, or regular polygons, the resistance distribution is even across equal segments.
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