Correct Answer - Option 3 : 1 mm
Concept:
Prandtl number Pr is defined as the ratio of momentum diffusivity to thermal diffusivity.
\(Pr = \frac{\nu }{\alpha } = \frac{{momentum\;diffusivity}}{{thermal\;diffusivity}}\)
\(Pr = \frac{{μ {C_p}}}{K} = \frac{{\left( {\frac{μ }{\rho }} \right)}}{{\left( {\frac{K}{{\rho {C_p}}}} \right)}}\)
In another way, we can define Prandtl number as, the ratio of the rate that viscous forces penetrate the material to the rate that thermal energy penetrates the material.
\(\frac{δ }{{{δ _T}}} = {\left( {Pr} \right)^{1/3}}\;\)
where δ is hydrodynamic boundary layer thickness and δT is thermal boundary layer thickness.
Calculation:
Given:
μ = 0.001 Pa.s, Cp = 1 kJ/kg.k, K = 1 W/m.k
Since, Prandtl number, \(Pr = \frac{{μ Cp}}{K}\)
So, \(Pr = \frac{{0.001 \times 1000}}{1} = 1\)
Since \(\frac{\delta }{{{\delta _T}}} = {\left( {Pr} \right)^{\frac{1}{3}}} = {\left( {1} \right)^{\frac{1}{3}}} = 1\)
∴ Thermal boundary layer thickness at the same location = 1mm