Electrical & Electronics Engineering / Three-Phase Two-Wattmeter
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LABORATORY 09 · ELECTRICAL & ELECTRONICS ENGINEERING

Three-Phase Two-Wattmeter lab report

A worked three-phase two-wattmeter lab report with sample observation tables, regression plots, calculations, and error analysis.

WORKED EXAMPLE · BENCHMARK OBSERVATIONS

A complete example electrical engineering laboratory report.

Simulated demonstration data.

This report illustrates formal electrical engineering data reduction, instrument calibration tares, and circuit parameter estimation. Replace its observations with your own experimental telemetry when preparing an electrical engineering laboratory report submission.

Student: __________________Student ID: __________________Course: __________________Date: __________________Partner: __________________Instructor: __________________

1. Title and aim

Three-Phase Balanced and Unbalanced Real Power Measurement Using the Two-Wattmeter Method. Measure total real power (P) and load power factor (cos φ) in balanced and unbalanced three-phase three-wire star/delta loads using Blondel's two-wattmeter method.

2. Abstract

Laboratory evaluation of Three-Phase Balanced and Unbalanced Real Power Measurement Using the Two-Wattmeter Method was conducted across six calibrated setpoints. Measured telemetry was linearized, yielding a correlation coefficient R² = 1.000000. The experimental parameter Three-Phase Power Scaling Coefficient was estimated as 1.4500 kW/(100/Ω), comparing against the reference benchmark of 1.4500 kW/(100/Ω) with a relative percentage deviation of 0.0000%.

3. Apparatus and fixed settings

4. Theory and graph choice

The experimental analysis of three-phase balanced and unbalanced real power measurement using the two-wattmeter method investigates the electrotechnical behavior of three-phase variable autotransformer & balanced load bank. This university laboratory module focuses on blondel's theorem, sum & difference wattmeter readings, phase angle calculation, establishing accurate mathematical transfer characteristics across standard operational domains.

P_3φ = 1.4500 · (100/R)

Plotting Conductance index 100/R (100/Ω) on the horizontal axis and Total measured active power P_3φ (kW) on the vertical axis yields a linear characteristic whose slope verifies the Three-Phase Two-Wattmeter analytical model.

5. Method

  1. Inspect all circuit connections, breadboard jumpers, and terminal blocks. Verify that instrument ground planes are tied to earth and execute zero tare on all digital meters.
  2. Energize the regulated supply, set baseline operating thresholds, and calibrate the conductance index using the precision standard reference meter.
  3. Increment the conductance index systematically across the designated experimental range (1.0 to 6.0 100/Ω), permitting thermal settling at each setpoint.
  4. Record the primary output metric (Total Measured Active Power P_3φ) alongside auxiliary telemetry. Verify waveform symmetry, DC offset, and harmonic integrity on the oscilloscope.
  5. Execute repeated forward and reverse sweeps to detect hysteresis, thermal drift, or non-linear saturation effects across the device under test (DUT).
  6. Reduce source excitation smoothly to zero, de-energize all primary supplies, discharge residual capacitive elements, and export raw telemetry to the data buffer.

6. Observations and calculation table

All electrical engineering observations use strictly controlled 64-bit IEEE 754 precision buffers. Residuals are computed relative to the ordinary least-squares regression line.

Table 1. Six simulated observations; x and y represent transformed electrical engineering metrics.
No.Per-Phase Conductance Index 100/R (100/Ω)Total Measured Active Power P_3φ (kW)Conductance index 100/R (100/Ω)Total measured active power P_3φ (kW)Fitted yResidual
11.01.451.00001.45001.45000.0000
22.02.92.00002.90002.90000.0000
33.04.353.00004.35004.35000.0000
44.05.84.00005.80005.80000.0000
55.07.255.00007.25007.25000.0000
66.08.76.00008.70008.70000.0000

Download the sample observations (CSV) ↓

7. Worked calculation for one observation

x = 1.0000; y = 1.4500; fitted_y = 1.4500 · x + 0.0000 = 1.4500

8. Graph, gradient and final calculation

0.751.091.852.682.954.284.055.875.157.476.259.06Conductance index 100/R (100/Ω)Total measured active power P_3φ (kW)

Circular markers represent empirical circuit observations. The solid line represents the ordinary least-squares linear fit.

x̄ = 3.5000; ȳ = 5.0750
Σ(x − x̄)² = 17.5000
Σ(x − x̄)(y − ȳ) = 25.3750
m = Σ(x − x̄)(y − ȳ) / Σ(x − x̄)² = 1.45000000
b = ȳ − mx̄ = 0.00000000
Three-Phase Power Scaling Coefficient = 1.45000 kW/(100/Ω)

9. Uncertainty and comparison

Percentage difference = |estimate − theoretical value| / |theoretical value| × 100 = 0.0000%.

For n = 6 observations, Σresidual² = 0.0000; s² = Σresidual²/(n − 2). Gradient standard error = √[s²/Σ(x − x̄)²] = 0.0000. Intercept standard error = √[s²(1/n + x̄²/Σ(x − x̄)²)] = 0.0000.

Propagating the fit parameters yields a fit standard error of 0.0000 kW/(100/Ω), with an ideal coefficient of determination R² = 1.000000.

Instrumental and regression uncertainty for Three-Phase Two-Wattmeter is constrained within 0.02% of full-scale calibration standards.

10. Result and discussion

Three-Phase Power Scaling Coefficient = 1.4500 kW/(100/Ω)
Theoretical reference value: 1.4500 kW/(100/Ω)

Experimental observations across all test trials demonstrate strict agreement with theoretical circuit models. OLS regression slope evaluated to 1.450000 with intercept 0.000000, validating the governing equation P_3φ = 1.4500 · (100/R) with R² = 1.000000.

11. Precautions and limitations

Assumes ideal linear operating conditions without thermal breakdown or non-linear core saturation Calibrated using the Three-Phase Variable Autotransformer & Balanced Load Bank under controlled temperature and 64-bit IEEE 754 precision instrumentation buffers. Ordinary least-squares regression yields R² > 0.99999.

12. Conclusion

The experimental determination of Three-Phase Balanced and Unbalanced Real Power Measurement Using the Two-Wattmeter Method confirmed the theoretical model within an experimental uncertainty of 0.0000%. The standard calibration protocol ensures reproducible laboratory characterization.

In-Depth Technical Supplement & Circuit Engineering Derivation

1. Title and Objective

Three-Phase Balanced and Unbalanced Real Power Measurement Using the Two-Wattmeter Method. Measure total real power (P) and load power factor (cos φ) in balanced and unbalanced three-phase three-wire star/delta loads using Blondel's two-wattmeter method. This formal laboratory report documents experimental data acquisition, mathematical model calibration, regression analysis, and error propagation for three-phase two-wattmeter.

2. Abstract

An experimental investigation of three-phase two-wattmeter was conducted using precision laboratory instrumentation across six systematic setpoints of conductance index ranging from 1.0 to 6.0 100/Ω. Measured total measured active power p_3φ data were logged using 6.5-digit digital multimeters and digital storage oscilloscopes. Ordinary least-squares regression yielded an empirical calibration line of P_3φ = 1.4500 · (100/R) with a coefficient of determination R² = 1.000000. The derived experimental parameter Three-Phase Power Scaling Coefficient was evaluated as 1.45 kW/(100/Ω), demonstrating complete agreement with theoretical benchmark expectations within 0.02% experimental error.

3. Experimental Apparatus & Standard Settings

  • Three-Phase Two-Wattmeter Precision Workstation: Provides regulated excitation, calibrated terminal access, and low-parasitic interconnects for blondel's theorem, sum & difference wattmeter readings, phase angle calculation.
  • True-RMS Digital Multimeter (6.5-digit Keysight / Fluke): Measures terminal voltages, branch currents, and precision DC/AC parameters with ±0.0035% baseline accuracy.
  • Dual-Channel Digital Storage Oscilloscope (100 MHz, 1 GSa/s): Captures time-domain waveforms, phase shifts, transient dynamics, and harmonic spectra for three-phase two-wattmeter.
  • Regulated Linear DC / AC Variable Power Source: Supplies low-noise, ripple-free voltage and current excitation with adjustable current limiting.
  • Calibrated Decade Resistance & Component Substitution Box: Provides precision 0.1% tolerance standard passive values to establish calibrated conductance index conditions.
  • Four-Terminal Kelvin Lead Wire & BNC Coaxial Cable Set: Minimizes lead resistance, inductive pickup, and ambient EMI interference across all test ports.
  • Environmental Ambient Conditions: Ambient laboratory temperature 23.5 ± 0.5 °C; relative humidity 45 ± 5%; atmospheric pressure 101.3 kPa.
  • Excitation Calibration Settings: Primary source stabilized within ±0.01% using closed-loop linear voltage regulation.

4. Theory & Graphical Coordinate Selection

According to the principles of three-phase two-wattmeter, the circuit response follows the linear transformation:

P_3φ = 1.4500 · (100/R)

To evaluate the intrinsic physical parameter (Three-Phase Power Scaling Coefficient), the experimental data are plotted with Conductance index 100/R (100/Ω) on the horizontal abscissa and Total measured active power P_3φ (kW) on the vertical ordinate. The gradient of the resulting least-squares linear line directly yields the parameter magnitude.

5. Step-by-Step Experimental Method

  1. Visual Inspection & Pre-Flight Zero Tare: Inspect all circuit connections, breadboard jumpers, and terminal blocks. Verify that instrument ground planes are tied to earth and execute zero tare on all digital meters.
  2. Excitation Source & Baseline Calibration: Energize the regulated supply, set baseline operating thresholds, and calibrate the conductance index using the precision standard reference meter.
  3. Systematic Parameter Variation & Settling: Increment the conductance index systematically across the designated experimental range (1.0 to 6.0 100/Ω), permitting thermal settling at each setpoint.
  4. Multi-Meter & Oscilloscope Waveform Acquisition: Record the primary output metric (Total Measured Active Power P_3φ) alongside auxiliary telemetry. Verify waveform symmetry, DC offset, and harmonic integrity on the oscilloscope.
  5. Cross-Validation & Redundant Trial Verification: Execute repeated forward and reverse sweeps to detect hysteresis, thermal drift, or non-linear saturation effects across the device under test (DUT).
  6. Shutdown, De-energization & Data Archival: Reduce source excitation smoothly to zero, de-energize all primary supplies, discharge residual capacitive elements, and export raw telemetry to the data buffer.

6. Raw Experimental Observations & Data Tabulation

All experimental observations were recorded under steady-state thermal and electrical equilibrium. The table below summarizes the recorded telemetry across the experimental domain.

Table 1. Experimental observation telemetry for Three-Phase Two-Wattmeter.
Trial # Per-Phase Conductance Index 100/R (100/Ω) Total Measured Active Power P_3φ (kW) Transformed x Transformed y Residual
11.01.451.0001.4500.000
22.02.92.0002.9000.000
33.04.353.0004.3500.000
44.05.84.0005.8000.000
55.07.255.0007.2500.000
66.08.76.0008.7000.000

7. Worked Calculation for Representative Observation

For Trial 3 (Conductance Index = 3.0 100/Ω):

x_3 = 3.0 100/Ω
y_3 = m \cdot x_3 + b = P_3φ = 1.4500 · 3.0
Derived Parameter Value = 1.45 kW/(100/Ω)

8. Regression Analysis, Gradient & Parameter Extraction

Ordinary least-squares (OLS) linear regression was performed across the six observation pairs. The regression statistics are summarized below:

Slope m = 1.4500 kW/(100/Ω)
Intercept b = Calculated baseline offset
Correlation Coefficient R² = 1.000000
Standard Error of Slope SE_m = ±0.00008 kW/(100/Ω)

9. Uncertainty Propagation & Comparison with Reference

Measurement uncertainty was calculated following the ISO Guide to the Expression of Uncertainty in Measurement (GUM). Type A uncertainty evaluated from observation residuals yielded u_A = 0.0002. Type B instrumental calibration uncertainty from the 6.5-digit multimeter was u_B = 0.0005. The combined expanded uncertainty at a 95% confidence interval (coverage factor k = 2) is:

\[ U = k \cdot \sqrt{u_A^2 + u_B^2} = 2 \cdot \sqrt{(0.0002)^2 + (0.0005)^2} = \pm 0.0011\text{ kW/(100/Ω)} \]

The experimental estimate of 1.45 kW/(100/Ω) agrees with the theoretical reference value (1.45 kW/(100/Ω)) within an absolute deviation of 0.015%, well within the expanded uncertainty band.

10. Engineering Discussion & Phenomenological Interpretations

The experimental results confirm the theoretical behavior of three-phase two-wattmeter. The linearity observed across all six test points validates the assumption of linear, bilateral network characteristics. Thermal drift was effectively suppressed by maintaining low duty cycles and utilizing precision metal-film components. The minor residual fluctuations observed are attributable to quantization resolution and Johnson–Nyquist thermal noise in the passive bridge elements.

11. Industrial Applications & Construction Practice

The electrotechnical principles demonstrated in this laboratory form the core foundation of numerous modern engineering systems, including:

  • Power Grid & Transmission Engineering: Network equivalent modeling, short-circuit current calculations, power factor correction capacitor banks, and substation protective relay coordination.
  • Consumer Electronics & Integrated Circuits: Analog front-end amplification, active Butterworth filtering, switching power supply voltage regulation, and precision ADC/DAC mixed-signal conversion.
  • Industrial Automation & Drives: Variable frequency motor speed control, servomechanism closed-loop feedback, electromechanical energy conversion, and industrial PLC signal conditioning.

12. Conclusion & Recommendations

The experimental investigation of Three-Phase Balanced and Unbalanced Real Power Measurement Using the Two-Wattmeter Method was completed with complete success. The linear regression model verified the governing transfer equation with R² = 1.000000. All experimental safety protocols and precision measurement guidelines were strictly observed. For future investigations, automated GPIB/USB telemetry acquisition and environmental temperature chamber testing are recommended to characterize high-temperature coefficients.

Simulated demonstration data.

This report presents simulated benchmark observations generated for demonstration and academic instruction purposes. When submitting coursework, replace all numerical values with your actual laboratory workbench observations.