Step 1: Understand the Prandtl number.
The Prandtl number is defined as:
\[
\text{Pr} = \frac{\nu}{\alpha},
\]
where:
- \( \nu \) is the momentum diffusivity (kinematic viscosity),
- \( \alpha \) is the thermal diffusivity.
For \( \text{Pr} = 0.01 \):
\[
\nu \ll \alpha.
\]
This means that the momentum diffusivity is much smaller than the thermal diffusivity.
Step 2: Boundary layer thicknesses.
The thickness of the boundary layer is inversely related to diffusivity. For small Prandtl numbers (\( \text{Pr} \ll 1 \)):
- The thermal boundary layer is much thicker than the momentum boundary layer because thermal diffusivity dominates.
Step 3: Evaluate the statements.
1. (A): The momentum diffusivity is much larger than the thermal diffusivity.
- This is incorrect because \( \nu \ll \alpha \) for \( \text{Pr} = 0.01 \).
2. (B): The thickness of the momentum boundary layer is much smaller than that of the thermal boundary layer.
- This is correct because \( \text{Pr} \ll 1 \) implies the thermal boundary layer is thicker than the momentum boundary layer.
3. (C): The thickness of the momentum boundary layer is much larger than that of the thermal boundary layer.
- This is incorrect because the opposite is true for \( \text{Pr} \ll 1 \).
4. (D): The momentum diffusivity is much smaller than the thermal diffusivity.
- This is correct because \( \nu \ll \alpha \) for \( \text{Pr} = 0.01 \).
Step 4: Conclusion.
The correct statements are:
(B) The thickness of the momentum boundary layer is much smaller than that of the thermal boundary layer, (D) The momentum diffusivity is much smaller than the thermal diffusivity.