ASTR 210 · Lecture 05

Aperture Photometry

Measurement design as much as calculation

Learning Goals

  1. Define instrumental magnitude and photometric zero point.
  2. Derive a zero point from one standard star and verify it against two others.
  3. Explain how aperture and sky-annulus choice bias a photometric measurement.

Reading anchor: OpenStax Astronomy 2e, Chapter 17.1 (the brightness of stars, magnitudes).

Why This Matters

Aperture photometry converts pixel counts into a calibrated brightness, but the same star can yield different reported magnitudes depending on aperture radius, sky-annulus placement, and how carefully the zero point was derived. Photometry is a measurement-design problem, not only an arithmetic one.

Opening Phenomenon

A photometric pipeline processes three standard stars in the same field and filter. If the zero point derived from one star is correct, it should reproduce the catalog magnitudes of the other two without further adjustment.

First question: what here is directly measured, and what is inferred from a model?

Terms for This Lecture

instrumental magnitude

Definition: A logarithmic measure computed directly from a background-subtracted detector count rate before absolute calibration.

Why it matters here: It places measured flux on a convenient relative scale that can be tied to catalog standards.

Relationships: The usual definition is \(m_{inst}=-2.5\log_{10}(C/t)\), and the calibrated magnitude adds a zero point and any needed color/extinction terms.

Boundary / common confusion: Instrumental magnitudes from different systems or nights are not directly comparable without calibration.

Evidence We Need to Explain

Model

Quantitative Tool

\[ m = -2.5\log_{10}(\text{rate}) + {\rm ZP} \]

Worked Example

  1. STD-A count rate = 150000/30 = 5000.0 counts/s.
  2. Solve for the zero point using the catalog magnitude: ZP = 10.21 + 2.5×log10(5000.0) = 10.21 + 9.247 = 19.457.
  3. Apply ZP to STD-B: rate = 2066.7 counts/s, predicted m = −2.5×log10(2066.7) + 19.457 = 11.169 (catalog: 11.17) — agreement to about 1 millimagnitudes.
  4. Apply ZP to STD-C: rate = 800.0 counts/s, predicted m = −2.5×log10(800.0) + 19.457 = 12.200 (catalog: 12.2) — agreement to about 0 millimagnitudes.
  5. Because both independent checks reproduce the catalog values to a few millimagnitudes, this zero point is internally consistent and can be applied to the unknown target in the same field.

Visual Reasoning

Use the aperture/annulus schematic and the zero-point check together.

  • Why must the sky annulus be placed outside the source aperture?
  • What would it mean if STD-B or STD-C fell far off the 1:1 line?
Lecture 05: Aperture Photometrysky annulusaperturecatalog V (mag)predicted V (mag)STD-A (defines ZP)STD-BSTD-CSTD-B and STD-C, held out of the zero-point fit, land on the 1:1 line to within a few millimagnitudes -- confirming ZP=19.457 is internally consistent.
Aperture and sky-annulus geometry, plus the zero-point verification against two independent standards.

Common Pitfall

Choosing an aperture radius too small (losing source flux to the wings of the point-spread function) or too large (including excess sky noise), then blaming the resulting magnitude error on "bad seeing" rather than measurement design.

Active Learning Segment

Using the STD-A-derived zero point above, predict the magnitude of a fourth star with 38,000 counts in 30 s, then discuss what would make you distrust the prediction.

Lab or Observing Connection

Lab 03 (Aperture Photometry) uses this exact standard-star table to derive and verify a zero point, then applies it to an unknown target.

Synthesis

Photometry is a measurement-design problem: aperture size, sky annulus, and zero-point derivation all shape the final calibrated brightness.

References