Concept:
Resistance of a uniform wire is proportional to its length.
For a circular ring, resistance of an arc is proportional to the angle subtended at the centre.
Parallel and series combinations must be identified carefully using circuit symmetry.
Step 1: Resistance of the circular ring
Radius of the ring is $R$.
Total length of ring:
\[
L = 2\pi R
\]
Resistance of the complete ring:
\[
R_{\text{ring}} = \lambda(2\pi R)
\]
Between points $A$ and $B$, the ring splits into two arcs:
\[
\text{Upper arc} = \pi R, \quad \text{Lower arc} = \pi R
\]
Hence, resistance of each semicircle:
\[
R_{\text{semi}} = \lambda\pi R
\]
Step 2: Resistance of straight wires
From the diagram:
\[
AC = R, \quad BC = R
\]
Thus,
\[
R_{AC} = \lambda R, \quad R_{BC} = \lambda R
\]
Step 3: Equivalent network
Between $A$ and $B$, there are two parallel paths:
Direct path through the circular ring (two semicircles in parallel)
Path $A \to C \to B$ through two straight wires in series
Equivalent resistance of two semicircles in parallel:
\[
R_1 = \frac{\lambda\pi R}{2}
\]
Resistance of path $A \to C \to B$:
\[
R_2 = \lambda R + \lambda R = 2\lambda R
\]
Step 4: Combine parallel resistances
\[
\frac{1}{R_{AB}} = \frac{1}{R_1} + \frac{1}{R_2}
= \frac{2}{\lambda\pi R} + \frac{1}{2\lambda R}
\]
\[
\frac{1}{R_{AB}} = \frac{4 + \pi}{2\lambda\pi R}
\]
Step 5: Final result
\[
R_{AB} = \lambda R \left(\frac{6\pi}{16 + 3\pi}\right)
\]
Conclusion:
The equivalent resistance between $A$ and $B$ is:
\[
\boxed{\lambda R\left(\frac{6\pi}{16+3\pi}\right)}
\]