Step 1: Recall Reynolds number formula.
The Reynolds number for flow is given by:
\[
Re = \frac{\rho \, V \, L}{\mu}
\]
where
- \(\rho\) = density of fluid,
- \(V\) = velocity of fluid,
- \(L\) = characteristic length,
- \(\mu\) = dynamic viscosity of fluid.
Step 2: Condition of the problem.
It is stated that the Reynolds number is kept constant. This means:
\[
\frac{\rho_1 V_1 L}{\mu_1} = \frac{\rho_2 V_2 L}{\mu_2}
\]
Since the characteristic length \(L\) is the same in both cases, it cancels out:
\[
\frac{\rho_1 V_1}{\mu_1} = \frac{\rho_2 V_2}{\mu_2}
\]
Step 3: Substitute values for case 1 (original liquid).
- \(\rho_1 = 1 \, \text{g/cm}^3\)
- \(\mu_1 = 0.01 \, \text{Poise}\)
- \(V_1 = 1 \, \text{cm/s}\)
So,
\[
\frac{1 \times 1}{0.01} = 100
\]
Step 4: Write the equation for case 2 (new liquid).
- \(\rho_2 = 1.25 \, \text{g/cm}^3\)
- \(\mu_2 = 0.015 \, \text{Poise}\)
- \(V_2 = ?\)
From the relation:
\[
\frac{\rho_1 V_1}{\mu_1} = \frac{\rho_2 V_2}{\mu_2}
\]
\[
100 = \frac{1.25 \, V_2}{0.015}
\]
Step 5: Solve for \(V_2\).
\[
100 \times 0.015 = 1.25 \, V_2
\]
\[
1.5 = 1.25 \, V_2
\]
\[
V_2 = \frac{1.5}{1.25} = 1.2
\]
Step 6: Final answer.
Thus, the characteristic velocity of the second liquid is:
\[
\boxed{1.2 \, \text{cm per second}}
\]