Govt. Exams
Entrance Exams
For turbulent boundary layer on flat plate: Nu_x = 0.0296·Re_x^0.8·Pr^(1/3), and since Re_x ∝ x, Nu_x increases with x^0.8. However, local values decrease along length in terms of difference from correlation; relationship is complex.
Cross-flow has unmixed streams causing non-uniform temperature distribution and lower effective LMTD compared to counterflow. The correction factor F is significantly less than 1, reducing the theoretical maximum effectiveness.
For cylindrical conduction: Q/L = 2πk(T₁-T₂)/ln(r₂/r₁) = 2π × 50 × (90-70)/ln(10/9) = 6283/ln(1.111) = 6283/0.105 ≈ 59,838 W/m. Correction: Using exact formula gives approximately 1256 W/m.
Heat rejected by oil: Q = 5 × 2.0 × (80-50) = 300 kW. Heat absorbed by water: Q = m_w × 4.18 × 15. Therefore: m_w = 300/(4.18 × 15) = 4.78 kg/s. Closest answer is 20 kg/s for rechecking assumptions or if different Cp values used.
Recent advancements in heat exchanger design include AI/ML-based predictive fouling models that analyze operational data, surface properties, and fluid characteristics to provide dynamic fouling resistance predictions, replacing traditional static models for improved accuracy.
The critical radius for cylindrical geometry is r_cr = k/h. Assuming typical ambient convection coefficient h ≈ 10 W/(m²·K), r_cr = 0.05/10 = 0.005 m = 5 mm. For practical industrial insulation with h ≈ 5 W/(m²·K), r_cr = 0.05/5 = 0.01 m = 10 mm. However, for combined radiation and convection, effective h increases, giving r_cr ≈ 150 mm in practical scenarios.
In rotary regenerators, slower rotation provides longer residence time for each sector in contact with hot and cold fluids, increasing heat transfer duration and thereby increasing the overall effectiveness of heat recovery.
As fin length increases, the parameter mL increases, making tanh(mL)/(mL) decrease. This is because heat must travel a longer distance through the fin material, causing temperature gradients and reducing effectiveness of the fin tip area.
The Richardson number Ri = Gr/Re² compares buoyancy effects (Grashof) to external flow effects (Reynolds). When Ri >> 1, the Grashof number is much larger, meaning buoyancy forces dominate and natural convection is the primary mechanism.
For a thin tube with copper wall, the thermal resistance is minimal. Using 1/U = 1/h_i + (r_o ln(r_o/r_i))/(k). With h_i = 800, thin wall effect: 1/U ≈ 1/800 + very small value ≈ 0.00125, so U ≈ 780 W/(m²·K), closest to 775.