A circular coil of single turn has a resistance of 20 Ω. Which one of the following is the correct value for resistance between the ends of any diameter of the coil?
5 Ω
The question asks for the resistance between the ends of any diameter of a circular coil that has a total resistance of 20 Ω for its single turn.
When we consider the resistance between two points on a circular coil that are diametrically opposite (i.e., at the ends of a diameter), the coil is effectively split into two equal halves.
Let the total resistance of the single-turn coil be \(R_{total}\). We are given \(R_{total} = 20 \, \Omega\).
Since the coil is uniform, the resistance of any part of the coil is proportional to its length. When considering the resistance across a diameter, the coil is divided into two semicircular sections. Each semicircular section is half the total length of the coil.
Therefore, the resistance of each semicircular section will be half of the total resistance:
\(R_{half} = \frac{R_{total}}{2}\)
\(R_{half} = \frac{20 \, \Omega}{2} = 10 \, \Omega\)
Now, these two semicircular sections are connected between the same two points (the ends of the diameter). This means they are connected in parallel.
To find the equivalent resistance of two resistors connected in parallel, we use the formula:
\(R_{eq} = \frac{R_1 \times R_2}{R_1 + R_2}\)
In this case, \(R_1 = R_{half} = 10 \, \Omega\) and \(R_2 = R_{half} = 10 \, \Omega\).
Substituting these values:
\(R_{eq} = \frac{10 \, \Omega \times 10 \, \Omega}{10 \, \Omega + 10 \, \Omega}\)
\(R_{eq} = \frac{100 \, \Omega^2}{20 \, \Omega}\)
\(R_{eq} = 5 \, \Omega\)
So, the equivalent resistance between the ends of any diameter of the coil is 5 Ω.
| Component | Resistance | Connection Type |
|---|---|---|
| Full Coil | 20 Ω | N/A |
| Semicircular Half 1 | 10 Ω | Parallel |
| Semicircular Half 2 | 10 Ω | Parallel |
| Equivalent Resistance (Across Diameter) | 5 Ω | Result |
| Concept | Description |
|---|---|
| Resistance (R) | Opposition to electric current flow, measured in Ohms (\(\Omega\)). |
| Resistance Proportional to Length | For a uniform conductor, \(R \propto L\). If length is halved, resistance is halved. |
| Parallel Connection | Components connected across the same two points. Equivalent resistance is less than the smallest individual resistance. Formula for two resistors: \(R_{eq} = \frac{R_1 R_2}{R_1 + R_2}\). |
| Series Connection | Components connected end-to-end, current flows through each sequentially. Equivalent resistance is the sum of individual resistances. \(R_{eq} = R_1 + R_2 + ...\) |
The resistance of a conductor depends on its material, length, and cross-sectional area. The formula is \(R = \rho \frac{L}{A}\), where:
In this circular coil problem, the material (\(\rho\)) and cross-sectional area (\(A\)) are uniform throughout the coil. Therefore, the resistance is directly proportional to the length (\(L\)). When the coil is split into two equal halves by the diameter, the length of each half is \(L_{total}/2\), and consequently, the resistance of each half is \(R_{total}/2\).
Connecting these two halves across the diameter forms a parallel circuit because the current entering at one end of the diameter splits and flows through both semicircular paths simultaneously, recombining at the other end of the diameter. This parallel arrangement of the two 10 Ω resistances results in the lower equivalent resistance of 5 Ω.
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