When a resistor of resistance R is connected across a.c. the terminal p.d. of the cell is reduced to three-quarter its e.m.f. The cell’s internal resistance in terms of R is
Given that the terminal potential difference (p.d.) of the cell is reduced to three-quarters of its e.m.f. when a resistor \( R \) is connected, we can express this as:
\(V = \frac{3}{4} E\)
The relationship between terminal voltage \( V \), e.m.f. \( E \), internal resistance \( r \), and current \( I \) is given by:
\(V = E - Ir\)
The current \( I \) can be expressed as: \(I = \frac{V}{R}\)
Substituting for \( I \) in the voltage equation:
\(V = E - \left(\frac{V}{R}\right) r\)
Substituting \( V = \frac{3}{4} E \):
\(\frac{3}{4} E = E - \left(\frac{\frac{3}{4} E}{R}\right) r\)
Rearranging gives: \(\frac{3}{4} E = E - \frac{3Er}{4R}\)
Simplifying: \(\frac{3}{4} E - E = -\frac{3Er}{4R}\)
This leads to: \(-\frac{1}{4} E = -\frac{3Er}{4R}\)
Dividing both sides by \( -E \): \(\frac{1}{4} = \frac{3r}{4R}\)
Cross-multiplying results in: \(R = 3r\)
Finally, solving for \( r \): \(r = \frac{R}{3}\).
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