The viscosity \( \eta \) of a polymer is related to its molecular weight by the empirical equation:
\[
\eta = K M^n
\]
where \( M \) is the molecular weight and \( K \) and \( n \) are constants. The relationship for the viscosity of two polymers with different molecular weights is:
\[
\frac{\eta_2}{\eta_1} = \left( \frac{M_2}{M_1} \right)^n
\]
Given:
- \( \eta_1 = 8.0 \times 10^3 \) Pa·s, \( M_1 = 250 \times 10^3 \) g/mol,
- \( M_2 = 500 \times 10^3 \) g/mol,
- \( M_c = 35 \times 10^3 \) g/mol, and
- Using \( n = 0.8 \) (for polystyrene),
\[
\frac{\eta_2}{8.0 \times 10^3} = \left( \frac{500 \times 10^3}{250 \times 10^3} \right)^{0.8}
\]
Solving:
\[
\eta_2 \approx 8.0 \times 10^3 \times (2)^{0.8} \approx 8.0 \times 10^3 \times 1.741 \approx 13.9 \times 10^3 \, \text{Pa·s}.
\]
Thus, the viscosity will be approximately \( 14 \times 10^3 \) Pa·s.