(i) Relationship between R′ and R:
The resistance R of a conductor is defined as:
\(R = \frac {ρ l}{A}\)
If the length is doubled to 2l, and assuming constant volume, the cross-sectional area A becomes A/2. Consequently:
\(R′ = \frac {ρ (2l)}{(A/2) }= \frac {4ρ l}{A} = 4R\)
Therefore,\(R^′ = 4R.\)
(ii) Relationship between v′d and vd:
Drift velocity vd is expressed as:
\(v_d =\frac{I}{(neA)}\)
When the length is doubled, the current I remains constant (assuming an ideal cell), while the cross-sectional area A is halved. Thus:
\(v^′_d = 2v_d\)
Hence,\(v^′_d = 2v_d\).