Gas Meter Test Equipment: Synchronize Register Images with the Reference Volume

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Gas Meter Test Equipment: Synchronize Register Images with the Reference Volume

Abstract

An automated gas meter bench can recognize a register correctly and still pair that reading with the wrong reference interval. Chen, Shen and Wang describe a diaphragm gas meter verification bench that synchronizes camera capture with a bell-prover encoder at both endpoints. The design separately corrects the reference volume to the pressure and temperature at the meter inlet. This article examines the timing and state corrections, reproduces the authors' static-versus-dynamic comparison at two flow points, and explains how to inspect the supporting records. The case shows why a bench acceptance test should check paired images and counts as well as the final error calculation.

Background and research question

A gas meter test compares the volume registered by the meter with a reference volume. With an optical system, the test obtains the registered volume from the difference between two image readings. If the reference begins counting before the first image or continues after the second, the two differences cover different intervals. The discrepancy can affect the calculated error even if each camera image is read correctly and the reference volume is traceable. The same separation is needed when diagnosing a test run. A disagreement could come from register recognition, event timing, gas-state correction or the meter under test.
Chen, Shen and Wang addressed the timing question in the design of an automated bench for diaphragm meters [1]. The engineering question is how the bench makes the register readings and reference counts describe the same measurement interval. A second question is how much evidence their comparison provides about the operation of that design.

Apparatus and synchronized readings

The prototype uses a bell prover with a photoelectric bidirectional encoder. A camera photographs the meter register. A programmable controller collects the encoder and transducer data and controls the air path and related actuators, while the host processes the images and stores the results. The paper describes pressure and temperature measurements at the reference and at the meter inlet. These measurements are inputs to the reference correction.
After the selected flow has been established, a shared trigger initiates the start image and reference counting. The end image is captured when the target interval is reached, with the encoder count ending at the corresponding event. In an acceptance record, both images should be linked to their matching reference counts. Such a link matters more than two isolated timestamps because the user needs to recover the actual measurement pair at each endpoint.
The source also reports that the user enters the meter identification, selected flow point and number of verification runs before the test. Those settings are useful when a lab reviews saved files later. A record that ties the images, encoder readings and settings to one run is easier to audit than a folder of frames and a separate spreadsheet of errors.
Figure 1. Arrangement of the verification bench, redrawn in English from Chen, Shen and Wang [1], Figure 1 (PDF p. 1, print p. 28).
Bell prover and inlet valve supplying three illustrated diaphragm-meter stations with cameras and pneumatic clamps.
Figure 2. Monitoring and control block diagram, redrawn in English from Chen, Shen and Wang [1], Figure 2 (PDF p. 2, print p. 29).
Host computer, camera and PLC connections for the verification bench, including the encoder, valves and transducers.
Figure 3. Controller verification sequence, redrawn in English from Chen, Shen and Wang [1], Figure 3 (PDF p. 2, print p. 29).
Controller decisions and repeated flow-point tests linking the starting and ending register images to encoder counts.

Data reduction and gas-state correction

The authors calculate the single-run indication error as a percentage.
δ = [(Vm − Vref) / Vref] × 100% (1)
Vm is the volume indicated by the meter over the captured interval, and Vref is the reference volume expressed at the meter inlet state. The source uses the following relation to convert the indicated bell volume Vs.
Vref = Vs × (ps × Tm) / (pm × Ts) (2)
The suffix s refers to the bell and m to the meter inlet. Pressures ps and pm are absolute and stated in pascals. Temperatures Ts and Tm are thermodynamic temperatures in kelvin. The volumes in the equation are in dm³. Matching the endpoints determines what volume interval is compared. The pressure and temperature relation determines the state in which the reference volume is expressed. One calculation cannot compensate for an error in the other.

Experimental comparison

The authors used static manual and dynamic image-based readings for the same G2.5 meter. The paper gives two displayed readings for each method at 4.0 m³/h and 0.8 m³/h. The last column preserves the reported difference. It describes the method comparison and does not represent an error of an individual reading.
Flow point
Flow (m³/h)
Static error (%)
Dynamic error (%)
Reported mean difference (percentage points)
qmax
4.0
0.46, 0.37
0.36, 0.40
0.04
0.2qmax
0.8
0.96, 1.04
1.07, 1.15
0.11
Table. Static and dynamic indication-error readings for one G2.5 meter. Values are transcribed from Chen, Shen and Wang [1], Table 1.
At 4.0 m³/h, the average of the displayed static readings is 0.415% and that of the dynamic readings is 0.380%. Their absolute difference is 0.035 percentage points using the displayed inputs. The paper gives 0.04 in the difference column. At 0.8 m³/h, the displayed means are 1.00% and 1.11%, a difference of 0.11 percentage points. Retaining the displayed readings beside the rounded report makes both comparisons auditable.

Discussion, conclusion and outlook

The authors report an expanded uncertainty of 0.20% at k = 2 for the research bench. This figure describes the stated uncertainty of the bench. The table compares two acquisition methods on one meter and does not give an optical recognition success rate or an independently measured trigger delay. It supports the feasibility of pairing the measurements in the reported setup. It leaves open how the system behaves when the register is dirty, a digit is in transition, a capture is missed, or multiple stations share controls.
For a bench selection or acceptance review, specify which evidence the machine must retain for each run: both register frames, the corresponding reference counts, the pressure and temperature records, and the calculated error. A follow-on verification could deliberately test difficult register positions and confirm how the system identifies a missing or ambiguous capture. Testing several flow points, meter types and bench positions would give a stronger basis for judging repeatability beyond the reported specimen.

Notes

qmax is the tested meter's maximum flow. Reported differences and editorial differences calculated from displayed values are identified separately. The original bench and trial belong to the authors' institution.

References and Image Sources

[1] Chen, C., Shen, Q., and Wang, C. (2011). "Design of a diaphragm gas meter verification bench based on image recognition". Industrial Metrology, 21(4), pp. 28–29 and 35. Equations (1)–(2), Figures 1–3 and Table 1. Figures 1–3 are original English redraws of the source diagrams. https://doi.org/10.13228/j.boyuan.issn1002-1183.2011.04.003
Cover photo: Science History Institute, accession 2003.902.104, photographer unidentified. Mrs. M. K. Murray demonstrating a nitrometer in a laboratory. Public Domain Mark 1.0 per the source record. Editorial photo crop and title layout. https://commons.wikimedia.org/wiki/File:THC_2003.902.104_Mrs._M._K._Murray_Nitrometer.jpg