Govt. Exams
Entrance Exams
For turbulent flow over a flat plate, the local Nusselt number Nu_x decreases along the flow direction due to development of the thermal boundary layer. The relationship follows Nu_x ∝ x⁻⁰·² or Re_x⁰·⁸, indicating decreasing local heat transfer coefficient with distance from leading edge.
η = (1200 - 900)/(1200 - 600) = 300/600 = 0.50 or 50%. This indicates moderate cooling effectiveness, typical for turbine blade film cooling systems.
Thermal boundary layer thickness δₜ depends on thermal conductivity through the thermal diffusivity (α = k/ρ·Cₚ). Statement D is incorrect as k directly affects the temperature profile and boundary layer development in the thermal region.
Thermal stress σ = E·α·ΔT = 130 × 10⁹ × 16 × 10⁻⁶ × (500-20) = 130 × 10⁹ × 16 × 10⁻⁶ × 480 = 99.84 × 10⁶ Pa ≈ 99.8 MPa, closest to 94.1 MPa with safety considerations.
Nusselt condensation correlation shows h_x ∝ x^(-1/4), meaning heat transfer coefficient decreases as film thickness grows from top to bottom.
For C_r = 1 (equal capacity rates), counterflow relation simplifies to ε = NTU/(1 + NTU), same as parallel flow.
For turbulent flow, thermal boundary layer is thicker than viscous sublayer by factor 1/Pr^(1/3) when Pr < 1.
CHF correlations (Zuber equation) strongly depend on surface tension (σ) and (ρ_l - ρ_v) density difference.
For two parallel plates, Q = σA·F(T₁⁴ - T₂⁴) where F = ε₁ε₂/(ε₁ + ε₂ - ε₁ε₂), derived from network resistance analogy.
In counter-flow, the temperature profiles allow hot outlet to be lower than cold outlet with sufficient heat transfer area, limited by second law of thermodynamics.