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
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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.
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Key Skills:
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Safe operation of a shell-and-tube or concentric tube heat exchanger test rig.
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Precise measurement of inlet/outlet temperatures and flow rates of hot and cold fluids.
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Achieving and identifying steady-state conditions.
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Calculating
Uand comparing with theoretical values. -
Plotting performance curves (e.g.,
εvs.NTU). -
Comprehensive technical report writing and viva preparation.
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4.1 THEORETICAL FOUNDATION & GOVERNING EQUATIONS
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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).
$$ Q_h = \dot{m}_h C_{p,h} (T_{h,in} - T_{h,out}) = Q_c = \dot{m}_c C_{p,c} (T_{c,out} - T_{c,in}) $$
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Basic Conduction Law: Fourier's Law (for wall conduction).
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Convection Law: Newton's Law of Cooling.
$$ Q = U A \Delta T_{lm} $$
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Key Parameters:
- Log Mean Temperature Difference (LMTD): For constant
Uand flow rates.
- Log Mean Temperature Difference (LMTD): For constant
$$ \Delta T_{lm} = \frac{\Delta T_1 - \Delta T_2}{\ln(\Delta T_1 / \Delta T_2)} $$
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 $$\displaystyle C_{min} = \min(\dot{m}_h C_{p,h}, \dot{m}_c C_{p,c}) $$.
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Dimensionless Numbers (for flow analysis):
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Reynolds Number (Re): $$\displaystyle \text{Re} = \frac{\rho V D}{\mu} $$ (Indicates laminar/turbulent flow).
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Prandtl Number (Pr): $$\displaystyle \text{Pr} = \frac{\mu C_p}{k} $$ (Fluid property).
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Nusselt Number (Nu): $$\displaystyle \text{Nu} = \frac{h D}{k} $$ (Convective heat transfer coefficient).
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[!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
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Schematic: A typical setup includes:
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Test Section: Concentric tube or shell-and-tube heat exchanger.
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Hot Fluid Loop: Storage tank, immersion heater, pump, flow control valve, rotameter.
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Cold Fluid Loop: Similar to hot loop, often with a constant temperature source (e.g., cooling coil).
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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" -
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Instrument Specifications & Calibration:
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Thermocouples/RTDs: Range (0-100°C or higher), accuracy (±0.1°C or 0.5%).
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Rotameters: Range (LPH), calibration curve (linearity check).
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Stopwatch & Measuring Cylinder: For manual flow measurement (volumetric method). Least count (0.1 sec, 10 ml).
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Calibration: Compare instrument readings against a calibrated standard (e.g., standard thermometer). Note calibration certificates.
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4.3 EXPERIMENTAL PROCEDURE & OPERATION
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Pre-Experiment Checks:
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Check all electrical connections, earthing.
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Ensure all valves are closed, fluid levels in storage tanks are adequate.
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Verify no leaks in piping.
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Note ambient conditions.
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Step-by-Step Operation:
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Start cold water pump first. Set a constant flow rate.
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Start hot water pump. Set a desired flow rate (can be varied).
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Switch ON the heater. Set a constant power input (using variac/controller).
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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.
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Record:
T_h_in, T_h_out, T_c_in, T_c_out, flow rates (Q_h, Q_c), heater power input (W). -
Vary Parameters: Change either hot/cold flow rate or heater power. Repeat steps 4-5 for at least 4-5 different conditions.
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Shutdown: Switch OFF heater, then pumps after cooling.
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Safety Protocols:
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Wear gloves/face shield near hot surfaces/pipes.
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Ensure proper grounding for electrical heaters.
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Do not touch electrical panels with wet hands.
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Be cautious of pressurized water lines.
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[!TIP] Common Pitfall: Not waiting long enough for steady-state leads to erroneous
ΔTandQcalculations. 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
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Mass Flow Rate: If using volumetric flow (
V̇in m³/s), $$\displaystyle \dot{m} = \rho V̇ $$. Density (ρ) from temperature tables. -
Heat Transfer Rate: $$\displaystyle Q = \dot{m} C_p \Delta T $$. Use tabulated $$\displaystyle C_p $$ for water at mean temperature.
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LMTD Calculation: Use formula from 4.1. Identify
ΔT₁andΔT₂based on flow arrangement. -
Experimental U: $$\displaystyle U_{exp} = \frac{Q}{A \Delta T_{lm}} $$.
Ais heat transfer area (provided/calculated from tube dimensions). -
NTU & ε:
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Calculate $$\displaystyle C_h = \dot{m}_h C_{p,h} $$, $$\displaystyle C_c = \dot{m}_c C_{p,c} $$.
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Identify $$\displaystyle C_{min} $$ and $$\displaystyle C_{max} $$, $$\displaystyle C^* = C_{min}/C_{max} $$.
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$$\displaystyle NTU = \frac{U_{exp} A}{C_{min}} $$.
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Use effectiveness formula for the specific flow arrangement (parallel/counter) to find
ε_theofrom NTU andC*. -
Compare
ε_exp(fromQandQ_max) withε_theo.
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Graphical Analysis:
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Plot
Nuvs.Re(if velocity varied) to check flow regime. -
Plot
εvs.NTUfor experimental points and theoretical curve.
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4.6 RESULTS, DISCUSSION & ERROR ANALYSIS
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Presentation: Tabulate
U_exp,ε_exp,ε_theo. Plot required graphs. -
Discussion Points:
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U_expis usually lower than theoreticalU_calc(from individualhcorrelations) due to fouling, imperfect insulation, contact resistance. -
ε_expvs.ε_theo: Explain deviation due to heat loss to surroundings, inaccurateU, maldistribution. -
Counter-flow heat exchanger has higher
εthan parallel flow for sameNTUandC*. -
Effect of flow rate: Increasing flow rate generally increases
U(higherRe→ higherh) but may decreaseεifC_minincreases faster thanU A.
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Error Analysis:
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Systematic: Calibration error in thermocouples/rotameters, inaccurate
C_porA. -
Random: Parallax in reading, fluctuation at "steady-state".
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Heat Loss: Major source. Affects
Qbalance (Q_h ≠ Q_c). Insulation minimizes this. -
Uncertainty Propagation: Use formula for
z = f(x,y). E.g., $$\displaystyle \frac{\Delta U}{U} = \sqrt{ \left(\frac{\Delta Q}{Q}\right)^2 + \left(\frac{\Delta A}{A}\right)^2 + \left(\frac{\Delta (\Delta T_{lm})}{\Delta T_{lm}}\right)^2 } $$.
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4.7 LAB REPORT FORMAT & VIVA-VOCE PREPARATION
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Standard Report Structure:
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Title, Aim, Apparatus (with schematic).
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Theory (LMTD, NTU-ε method, formulas).
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Procedure (step-by-step, safety).
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Observation Tables (raw data).
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Calculations (show sample for one set).
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Final Results Table & Graphs.
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Discussion & Error Analysis.
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Conclusion (e.g., "Counter-flow is more effective.").
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Key Viva Questions & Answers:
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Q: What is the purpose of this experiment?
A: To determine the overall heat transfer coefficient
Uand effectivenessεof 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).
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Q: Why is LMTD used instead of simple ΔT?
A: Because
ΔTvaries along the length of the heat exchanger. LMTD is an averageΔTthat correctly represents the driving force for heat transfer in constant-Uconditions. -
Q: What are the major sources of error?
A: Heat loss to surroundings, inaccurate flow measurement, thermocouple calibration, assumption of constant
C_pandU. -
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.
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Q: What is the significance of the Nusselt number?
A: It is the dimensionless heat transfer coefficient.
Nu = 1means pure conduction;Nu > 1indicates convection enhancement. It relateshto conductive heat transfer across the fluid boundary layer.
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\boxed{U = \frac{Q}{A \Delta T_{lm}}} \quad \boxed{\varepsilon = \frac{Q}{Q_{max}}} \quad \boxed{NTU = \frac{U A}{C_{min}}}