xraytools.

Isotope Pattern

The distribution of molecular masses that the natural isotopic composition of the elements produces — the M, M+1, M+2 series a mass spectrum shows — together with the monoisotopic and average mass.

You supply
A chemical formula, in the same grammar every other page here uses. Whole atoms only: a pattern describes one molecule, so a fractional stoichiometry is refused rather than rounded. Write a charge into the formula (SO4^2-, Na+) and every mass becomes m/z, electron mass included.
Reading it
Abundances are relative to the tallest peak, which is not always the monoisotopic one — for tin or a polybrominated compound it is not. This is an exact combinatorial result, not a simulated spectrum: no resolution, no peak shape, no adducts and no fragmentation.

Worked examples: a nickel complex · dibromomethane · tin tetrachloride · a sulfate anion

Input

Write the charge into the formula if you want m/z: SO4^2-, [Fe(CN)6]^3-, Na+.

% of the tallest

Results

formula: SnCl4
monoisotopic mass: 259.77761
average mass: 260.5219
base peak: 259.7753

Pattern

Isotope pattern, 15 peaks. The table below carries the same numbers.0255075100251.7802 · 1.3 %253.7776 · 2.6 %255.7769 · 22.0 %256.7782 · 11.2 %257.7757 · 59.7 %258.7769 · 25.7 %259.7753 · 100.0 %260.7748 · 21.7 %261.7739 · 86.9 %262.7723 · 8.7 %263.7736 · 48.3 %264.7697 · 1.7 %265.7740 · 20.4 %267.7735 · 6.2 %269.7715 · 1.1 %251.78269.77
massnucleonsrelative / %abundance
251.7802 252 1.34 0.320 %
253.7776 254 2.62 0.626 %
255.7769 256 22.01 5.264 %
256.7782 257 11.18 2.673 %
257.7757 258 59.72 14.284 %
258.7769 259 25.66 6.137 %
259.7753 260 100.00 23.918 %
260.7748 261 21.70 5.190 %
261.7739 262 86.93 20.792 %
262.7723 263 8.66 2.071 %
263.7736 264 48.28 11.547 %
264.7697 265 1.66 0.397 %
265.7740 266 20.35 4.868 %
267.7735 268 6.20 1.484 %
269.7715 270 1.11 0.266 %

These are the relative abundances that follow from the natural isotopic composition of the elements — an exact combinatorial result, not a simulated spectrum. There is no instrument here: no resolution, no peak shape, no adducts and no fragmentation. Combinations with the same number of nucleons are shown as one peak at their abundance-weighted mass, which is what an instrument of ordinary resolving power sees; at high resolution several of these would split. Abundances are relative to the tallest peak, which is not always the monoisotopic one.