Equivalent resistance between the adjacent corners of a regular \(n\)-sided polygon of uniform wire of resistance \(R\) would be :
When calculating equivalent resistance in networks, break down the network into series and parallel combinations. Remember the formulas for equivalent resistance in series and parallel.
\(\frac{(n-1) R}{(2 n-1)}\)
\(\frac{(n-1) R}{n}\)
\(\frac{n^2 R}{n-1}\)
\(\frac{(n-1) R}{n^2}\)
Let \(r\) be the resistance of each side of the \(n\)-sided polygon. Since the total resistance of the wire is \(R\), and there are \(n\) sides, the resistance of each side is:
\[ r = \frac{R}{n} \]
When we consider the equivalent resistance between adjacent corners A and B, the polygon can be viewed as two resistors in parallel:
The equivalent resistance (\(R_{eq(AB)}\)) between A and B is given by the formula for parallel resistors:
\[ \frac{1}{R_{eq(AB)}} = \frac{1}{r} + \frac{1}{(n-1)r} \] \[ R_{eq(AB)} = \frac{r \times (n-1)r}{r + (n-1)r} = \frac{(n-1)r^2}{nr} = \frac{(n-1)r}{n} \]
Substitute \(r = \frac{R}{n}\) back into the equation:
\[ R_{eq(AB)} = \frac{(n-1)\left(\frac{R}{n}\right)}{n} = \frac{(n-1)R}{n^2} \]
The equivalent resistance between the adjacent corners of the polygon is:
\[ \frac{(n-1)R}{n^2} \quad \text{(Option 4)}. \]
Suppose resistance of each arm is r, then r=R/n
Req(AB)=R1+R2R1R2
r+(n−1)rr(n−1)r
=nrr(n−1)r
=nn−1r
=n2(n−1)R
The current passing through the battery in the given circuit, is:
Let A be a 3 × 3 matrix such that \(\text{det}(A) = 5\). If \(\text{det}(3 \, \text{adj}(2A)) = 2^{\alpha \cdot 3^{\beta} \cdot 5^{\gamma}}\), then \( (\alpha + \beta + \gamma) \) is equal to:
Current electricity is defined as the flow of electrons from one section of the circuit to another.
There are two types of current electricity as follows:
The current electricity whose direction remains the same is known as direct current. Direct current is defined by the constant flow of electrons from a region of high electron density to a region of low electron density. DC is used in many household appliances and applications that involve a battery.
The current electricity that is bidirectional and keeps changing the direction of the charge flow is known as alternating current. The bi-directionality is caused by a sinusoidally varying current and voltage that reverses directions, creating a periodic back-and-forth motion for the current. The electrical outlets at our homes and industries are supplied with alternating current.