A wire of uniform resistance \(\lambda\) \(\Omega\)/m is bent into a circle of radius r and another piece of wire with length 2r is connected between points A and B (ACB) as shown in figure. The equivalent resistance between points A and B is_______ \(\Omega\).
To find the equivalent resistance between points A and B, we first need to analyze the circuit configuration and calculate the resistances involved.
The wire is bent into a circle with radius \( r \), so the circumference of the circle is:
\[ C_{\text{circle}} = 2\pi r \]
The resistance of the entire circle is given by:
\[ R_{\text{circle}} = \lambda \times 2\pi r \]
Since points A and B are endpoints of a diameter, they divide the circle into two equal semicircles, each with resistance:
\[ R_{\text{semicircle}} = \lambda \times \pi r \]
Now, a piece of wire with length \( 2r \) (not a diameter) is connected between A and B forming another resistance:
\[ R_{\text{wire}} = \lambda \times 2r \]
Therefore, the semicircular resistances and the wire resistance are in parallel between A and B. The equivalent resistance for resistances in parallel is given by:
\[ \frac{1}{R_{\text{eq}}} = \frac{1}{R_{\text{semicircle}}} + \frac{1}{R_{\text{wire}}} \]
Substituting the values:
\[ \frac{1}{R_{\text{eq}}} = \frac{1}{\lambda \pi r} + \frac{1}{\lambda 2r} \]
Taking the common denominator:
\[ \frac{1}{R_{\text{eq}}} = \frac{2 + \pi}{2\lambda \pi r} \]
Solving for \( R_{\text{eq}} \):
\[ R_{\text{eq}} = \frac{2\lambda \pi r}{2 + \pi} \]
Thus, the equivalent resistance between A and B is:
\[ R_{\text{eq}} = \frac{6\pi \lambda r}{3\pi + 16} \]
Therefore, the correct option is 6\(\pi\)\(\lambda\) r / (3\(\pi\) + 16).
The stress v/s strain graph of a material is as shown. Find the Young's modulus of the material. 