Astm E562-19e1

To understand why point counting works, one must revisit stereology. ASTM E562 rests on the Delesse principle (1847), which states that the area fraction of a component on a two-dimensional plane through a material is an unbiased estimator of its volume fraction in the three-dimensional material.

Mathematically: [ V_V = A_A ]

Where:

But how do we measure ( A_A )? Instead of measuring areas directly (which is tedious), we use point counting: if you randomly place a grid of test points on the microstructure, the fraction of points that fall on the phase of interest approximates the area fraction.

[ A_A \approx P_P = \fracP_pP_t ]

Where:

Thus, by counting “hits” on the phase of interest, you directly estimate volume fraction. ASTM E562 formalizes this approach, specifying grid geometry, counting rules, and statistical targets.


Compared to E562-11, the E562-19e1 revision introduced:

No major technical changes were made from the 2011 to 2019 version—just refinements for clarity. astm e562-19e1


Choose a magnification that clearly distinguishes the phase of interest from all others. The rule of thumb: the spacing between grid points should be such that no feature is counted more than once, but small enough to sample the structure adequately. The standard suggests that the grid spacing should be roughly the size of the features of interest.

Most people assume that if you want to know how much of a material is porosity, ferrite, or graphite, you’d use a computer. But ASTM E562-19e1 defends a deceptively simple, manual method: the manual point count. It’s a testament to how systematic random sampling and basic statistics can outperform intuition—and even some automated systems—in metallography and materials science.

ASTM E562 requires reporting the 95% confidence interval. Compute:

[ s = \sqrt\frac\sum (\barV_V - V_V(field))^2n-1 ] To understand why point counting works, one must

[ 95%\ CI = \barV_V \pm \frac1.96 \times s\sqrtn ]

In 1976, ASTM International published the first version of E562. It was a humble document, outlining a method for determining the volume fraction of a phase in a microstructure using a point grid. Over the decades, it evolved, sharpened by the collective intellect of the world’s best microscopists.

By 2019, the standard had reached a level of precision that Aris Thorne had taken for granted.

The version in question, ASTM E562-19e1, is the "Standard Test Method for Determining Volume Fraction by Systematic Manual Point Count." The "e1" designation signifies a small but crucial editorial update—a refinement of language, a tightening of the screws to ensure that a lab in Germany and a lab in Ohio counted the exact same way. But how do we measure ( A_A )

It sounds bureaucratic. But in the world of materials science, bureaucracy is the only thing standing between a passenger plane and a debris field.

3 Comments, RSS

  1. astm e562-19e1
    Alex Wallace

    If you need to share libs across workstations (eg. at a company) you can add a repository located on a shared network drive once it’s mapped in Windows. This is how we can lock library versions and not have any problems!

    • astm e562-19e1
      A. Montanari

      The only concern about sharing libraries through network shared folders is that if someone has to go then on a macchine in a non-connected environment, then the opening of library manager will take really long time (at last since o.s. returns timeout network availability error)…
      Sometimes this is not the most efficient solution.

Your email address will not be published. Required fields are marked *

*

This site uses Akismet to reduce spam. Learn how your comment data is processed.