Step 1: Write the field at the centre.
A circular coil with $N$ turns carrying current $I$ makes a field at its centre: \[ B = \frac{\mu_0 N I}{2R} \] We must keep this field the same after the coil is changed.
Step 2: Track the wire and its resistance.
When the same wire is stretched to double its length, its cross section halves. Since resistance is $\rho L/A$, doubling $L$ and halving $A$ makes resistance go up by $4$ times: $R_w' = 4R_w$.
Step 3: Find the new number of turns.
Total wire length is $N(2\pi R)$. After stretching the length doubles and the new radius is $R' = R/3$: \[ N'(2\pi R') = 2N(2\pi R) \;\Rightarrow\; N'\left(\frac{R}{3}\right) = 2NR \;\Rightarrow\; N' = 6N \]
Step 4: Set the fields equal.
We want the new field to match the old: \[ \frac{\mu_0 N' I'}{2R'} = \frac{\mu_0 N I}{2R} \;\Rightarrow\; \frac{6N\,I'}{R/3} = \frac{N I}{R} \]
Step 5: Solve for the new current.
\[ 18 I' = I \;\Rightarrow\; I' = \frac{I}{18} \]
Step 6: Bring in the emf.
Using $I = E/R_w$ and $R_w' = 4R_w$: \[ \frac{E'}{4R_w} = \frac{1}{18}\frac{E}{R_w} \;\Rightarrow\; E' = \frac{4}{18}E = \frac{2E}{9} \] \[ \boxed{E' = \frac{2E}{9}} \]