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Morgan Taylor commited on
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Parent(s): 83880a1
edit readme for simplicity
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README.md
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@@ -120,7 +120,7 @@ python scripts/piv_vs_hwa_paper.py \
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```
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These exact commands, run against the shipped `reference_results/`, reproduce the paper
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figures
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CMU Serif and fall back to DejaVu). Quote the `--inst-labels` arguments exactly as shown
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(single quotes) so your shell does not eat the `$` characters.
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@@ -212,10 +212,7 @@ modes explore worker×thread trade-offs beyond the paper's sweep — see
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`pivtools-bench scaling --help`.)
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Throughput numbers are hardware-dependent: the paper's peak of 117 pairs/s was
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measured on a 192-core dual-EPYC node, and your core count sets your ceiling.
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scaling *shape* — near-linear until the memory bandwidth of the machine saturates —
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is the reproducible claim. On a cluster, wrap this same command in your scheduler
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of choice; nothing about it is scheduler-specific.
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## Tier 3 — re-derive the calibration models
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The synthetic boards are rendered through the same camera models that rendered the
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particle images, so the recovered calibration corresponds exactly to the imaging system
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(`calibration/stereo/ground_truth.npz` holds the true cameras
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stereo angle ≈ 89.9° vs the true 90.0°, RMS < 0.1 px). Detection writes proof figures
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beside the model.
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The experimental case uses a uniform scale-factor model rather than a fitted camera. The
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shipped model (`calibration/experimental/calibration/Cam1/scale_factor_planar/model/`)
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| `lplus` | wire length in wall units (45.6) |
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| `nu_air` | kinematic viscosity (m²/s) |
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The figure plots the uncorrected variance deliberately: at l+ ≈ 46 the wire attenuates
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the near-wall peak, and the comparison discusses that rather than hiding it behind a
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correction.
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## Image orientation
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There are no masks: the stereo renders fill the full frame and the planar images are
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full-field. Both synthetic geometries read physically — the channel wall is at the bottom
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row, fast flow at the top. The stereo renders have a single deterministic vertical flip
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composed into both the images and the calibration boards, so calibration and images are
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consistent. Do not flip anything downstream.
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## Provenance
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```
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These exact commands, run against the shipped `reference_results/`, reproduce the paper
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figures (fonts permitting: the scripts prefer
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CMU Serif and fall back to DejaVu). Quote the `--inst-labels` arguments exactly as shown
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(single quotes) so your shell does not eat the `$` characters.
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`pivtools-bench scaling --help`.)
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Throughput numbers are hardware-dependent: the paper's peak of 117 pairs/s was
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measured on a 192-core dual-EPYC node, and your core count sets your ceiling.
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## Tier 3 — re-derive the calibration models
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The synthetic boards are rendered through the same camera models that rendered the
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particle images, so the recovered calibration corresponds exactly to the imaging system
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(`calibration/stereo/ground_truth.npz`) holds the true cameras.
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The experimental case uses a uniform scale-factor model rather than a fitted camera. The
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shipped model (`calibration/experimental/calibration/Cam1/scale_factor_planar/model/`)
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| `lplus` | wire length in wall units (45.6) |
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| `nu_air` | kinematic viscosity (m²/s) |
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## Provenance
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