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ME-306 · Thermal Engg Lab/Quick Revision Short Notes

Thermal Engg Lab (ME-306) - Unit 4 Short Notes

ME-306: Thermal Engineering Lab - UNIT 4 Short Notes

(Based on Generic Blueprint - Assumed Theme: Heat Exchanger Performance Studies)


4.0 UNIT OVERVIEW & LEARNING OBJECTIVES

  • Purpose: To experimentally determine the performance of a heat exchanger (typically parallel flow and counter flow), calculate the Overall Heat Transfer Coefficient (U), and validate theoretical LMTD and Effectiveness-NTU methods.

  • Key Skills:

    • Safe operation of a shell-and-tube or concentric tube heat exchanger test rig.

    • Precise measurement of inlet/outlet temperatures and flow rates of hot and cold fluids.

    • Achieving and identifying steady-state conditions.

    • Calculating U and comparing with theoretical values.

    • Plotting performance curves (e.g., ε vs. NTU).

    • Comprehensive technical report writing and viva preparation.


4.1 THEORETICAL FOUNDATION & GOVERNING EQUATIONS

  • Fundamental Law: First Law of Thermodynamics for a control volume (steady flow energy equation).

    • Heat lost by hot fluid = Heat gained by cold fluid (assuming no losses).

$$ Q_h = \dot{m}_h C_{p,h} (T_{h,in} - T_{h,out}) = Q_c = \dot{m}_c C_{p,c} (T_{c,out} - T_{c,in}) $$

  • Basic Conduction Law: Fourier's Law (for wall conduction).

  • Convection Law: Newton's Law of Cooling.

$$ Q = U A \Delta T_{lm} $$

  • Key Parameters:

    • Log Mean Temperature Difference (LMTD): For constant U and flow rates.

$$ \Delta T_{lm} = \frac{\Delta T_1 - \Delta T_2}{\ln(\Delta T_1 / \Delta T_2)} $$

    where $$\displaystyle \Delta T_1 $$ and $$\displaystyle \Delta T_2 $$ are temperature differences at each end.

*   **Overall Heat Transfer Coefficient (U):** Represents total resistance to heat transfer.

$$ \frac{1}{U A} = \frac{1}{h_h A_h} + \frac{t_w}{k_w A_w} + \frac{1}{h_c A_c} $$

*   **Effectiveness (ε):** Actual heat transfer vs. maximum possible.

$$ \varepsilon = \frac{Q}{Q_{max}} = \frac{\dot{m}_c C_{p,c} (T_{c,out} - T_{c,in})}{\dot{m}_c C_{p,c} (T_{h,in} - T_{c,in})} \quad (\text{for } C_{min} = C_c) $$

*   **NTU Method:** Number of Transfer Units.

$$ NTU = \frac{U A}{C_{min}} $$

    where $$\displaystyle C_{min} = \min(\dot{m}_h C_{p,h}, \dot{m}_c C_{p,c}) $$.
  • Dimensionless Numbers (for flow analysis):

    • Reynolds Number (Re): $$\displaystyle \text{Re} = \frac{\rho V D}{\mu} $$ (Indicates laminar/turbulent flow).

    • Prandtl Number (Pr): $$\displaystyle \text{Pr} = \frac{\mu C_p}{k} $$ (Fluid property).

    • Nusselt Number (Nu): $$\displaystyle \text{Nu} = \frac{h D}{k} $$ (Convective heat transfer coefficient).

[!TIP] Exam Focus: Be prepared to derive LMTD for parallel vs. counter-flow configurations. Know the formula for ε for both flow arrangements from the NTU-effectiveness method.


4.2 APPARATUS & INSTRUMENTATION

  • Schematic: A typical setup includes:

    1. Test Section: Concentric tube or shell-and-tube heat exchanger.

    2. Hot Fluid Loop: Storage tank, immersion heater, pump, flow control valve, rotameter.

    3. Cold Fluid Loop: Similar to hot loop, often with a constant temperature source (e.g., cooling coil).

    4. Measurement Points: Temperature sensors (Thermocouples/RTDs) at all inlets and outlets. Pressure gauges (optional). Flow meters (Rotameters or measuring cylinder+stopwatch).

    DiagramSEARCH: " concentric tube heat exchanger experimental setup diagram labeled"
  • Instrument Specifications & Calibration:

    • Thermocouples/RTDs: Range (0-100°C or higher), accuracy (±0.1°C or 0.5%).

    • Rotameters: Range (LPH), calibration curve (linearity check).

    • Stopwatch & Measuring Cylinder: For manual flow measurement (volumetric method). Least count (0.1 sec, 10 ml).

    • Calibration: Compare instrument readings against a calibrated standard (e.g., standard thermometer). Note calibration certificates.


4.3 EXPERIMENTAL PROCEDURE & OPERATION

  • Pre-Experiment Checks:

    1. Check all electrical connections, earthing.

    2. Ensure all valves are closed, fluid levels in storage tanks are adequate.

    3. Verify no leaks in piping.

    4. Note ambient conditions.

  • Step-by-Step Operation:

    1. Start cold water pump first. Set a constant flow rate.

    2. Start hot water pump. Set a desired flow rate (can be varied).

    3. Switch ON the heater. Set a constant power input (using variac/controller).

    4. Wait for Steady-State: Monitor all 4 temperature readings. When they fluctuate less than ±0.2°C for 5-10 minutes, steady-state is reached.

    5. Record: T_h_in, T_h_out, T_c_in, T_c_out, flow rates (Q_h, Q_c), heater power input (W).

    6. Vary Parameters: Change either hot/cold flow rate or heater power. Repeat steps 4-5 for at least 4-5 different conditions.

    7. Shutdown: Switch OFF heater, then pumps after cooling.

  • Safety Protocols:

    • Wear gloves/face shield near hot surfaces/pipes.

    • Ensure proper grounding for electrical heaters.

    • Do not touch electrical panels with wet hands.

    • Be cautious of pressurized water lines.

[!TIP] Common Pitfall: Not waiting long enough for steady-state leads to erroneous ΔT and Q calculations. Always confirm stability before recording data.


4.4 DATA ACQUISITION & TABULATION

  • Observation Table Format:
S.No \dot{m}_h (kg/s) \dot{m}_c (kg/s) T_{h,in} (°C) T_{h,out} (°C) T_{c,in} (°C) T_{c,out} (°C) ΔT_1 (°C) ΔT_2 (°C)
1 ... ... ... ... ... ... ... ...
2 ... ... ... ... ... ... ... ...
  • Derived Quantities Table (Calculated):
S.No Q_h (W) Q_c (W) ΔT_{lm} (°C) U_{exp} (W/m²K) C_h (W/K) C_c (W/K) C_{min} NTU ε_{exp}
  • Note: Record multiple readings (2-3) for each steady-state point to estimate average and random error.

4.5 DATA ANALYSIS & CALCULATIONS

  1. Mass Flow Rate: If using volumetric flow (V̇ in m³/s), $$\displaystyle \dot{m} = \rho V̇ $$. Density (ρ) from temperature tables.

  2. Heat Transfer Rate: $$\displaystyle Q = \dot{m} C_p \Delta T $$. Use tabulated $$\displaystyle C_p $$ for water at mean temperature.

  3. LMTD Calculation: Use formula from 4.1. Identify ΔT₁ and ΔT₂ based on flow arrangement.

  4. Experimental U: $$\displaystyle U_{exp} = \frac{Q}{A \Delta T_{lm}} $$. A is heat transfer area (provided/calculated from tube dimensions).

  5. NTU & ε:

    • Calculate $$\displaystyle C_h = \dot{m}_h C_{p,h} $$, $$\displaystyle C_c = \dot{m}_c C_{p,c} $$.

    • Identify $$\displaystyle C_{min} $$ and $$\displaystyle C_{max} $$, $$\displaystyle C^* = C_{min}/C_{max} $$.

    • $$\displaystyle NTU = \frac{U_{exp} A}{C_{min}} $$.

    • Use effectiveness formula for the specific flow arrangement (parallel/counter) to find ε_theo from NTU and C*.

    • Compare ε_exp (from Q and Q_max) with ε_theo.

  6. Graphical Analysis:

    • Plot Nu vs. Re (if velocity varied) to check flow regime.

    • Plot ε vs. NTU for experimental points and theoretical curve.


4.6 RESULTS, DISCUSSION & ERROR ANALYSIS

  • Presentation: Tabulate U_exp, ε_exp, ε_theo. Plot required graphs.

  • Discussion Points:

    • U_exp is usually lower than theoretical U_calc (from individual h correlations) due to fouling, imperfect insulation, contact resistance.

    • ε_exp vs. ε_theo: Explain deviation due to heat loss to surroundings, inaccurate U, maldistribution.

    • Counter-flow heat exchanger has higher ε than parallel flow for same NTU and C*.

    • Effect of flow rate: Increasing flow rate generally increases U (higher Re → higher h) but may decrease ε if C_min increases faster than U A.

  • Error Analysis:

    • Systematic: Calibration error in thermocouples/rotameters, inaccurate C_p or A.

    • Random: Parallax in reading, fluctuation at "steady-state".

    • Heat Loss: Major source. Affects Q balance (Q_h ≠ Q_c). Insulation minimizes this.

    • Uncertainty Propagation: Use formula for z = f(x,y). E.g., $$\displaystyle \frac{\Delta U}{U} = \sqrt{ \left(\frac{\Delta Q}{Q}\right)^2 + \left(\frac{\Delta A}{A}\right)^2 + \left(\frac{\Delta (\Delta T_{lm})}{\Delta T_{lm}}\right)^2 } $$.


4.7 LAB REPORT FORMAT & VIVA-VOCE PREPARATION

  • Standard Report Structure:

    1. Title, Aim, Apparatus (with schematic).

    2. Theory (LMTD, NTU-ε method, formulas).

    3. Procedure (step-by-step, safety).

    4. Observation Tables (raw data).

    5. Calculations (show sample for one set).

    6. Final Results Table & Graphs.

    7. Discussion & Error Analysis.

    8. Conclusion (e.g., "Counter-flow is more effective.").

  • Key Viva Questions & Answers:

    • Q: What is the purpose of this experiment?

      A: To determine the overall heat transfer coefficient U and effectiveness ε of a heat exchanger, compare parallel and counter-flow performance, and validate LMTD/NTU methods.

    • Q: How do you ensure steady-state? How do you know it's reached?

      A: By maintaining constant flow rates and heater power. Steady-state is reached when all 4 temperature readings stabilize (change < 0.2°C over 5-10 min).

    • Q: Why is LMTD used instead of simple ΔT?

      A: Because ΔT varies along the length of the heat exchanger. LMTD is an average ΔT that correctly represents the driving force for heat transfer in constant-U conditions.

    • Q: What are the major sources of error?

      A: Heat loss to surroundings, inaccurate flow measurement, thermocouple calibration, assumption of constant C_p and U.

    • Q: Explain the working principle of a rotameter.

      A: A variable area flow meter. Fluid flows up a tapered tube, lifting a float. At equilibrium, float position indicates flow rate on a calibrated scale.

    • Q: What is the significance of the Nusselt number?

      A: It is the dimensionless heat transfer coefficient. Nu = 1 means pure conduction; Nu > 1 indicates convection enhancement. It relates h to conductive heat transfer across the fluid boundary layer.

\boxed{U = \frac{Q}{A \Delta T_{lm}}} \quad \boxed{\varepsilon = \frac{Q}{Q_{max}}} \quad \boxed{NTU = \frac{U A}{C_{min}}}

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