Decay Simulator: Osmium-170
General data
| Element name | Osmium |
|---|---|
| Chemical symbol | Os |
| Atomic number Z | 76 |
| Isotope name (symbol) | Osmium-170 (Os-170) |
| Neutron number N | 94 |
| Mass number A=Z+N | 170 |
Interactive radioactive decay simulation of Osmium-170: atom-by-atom decay, full decay chain, charts of nuclei count and activity.
| Half-life | 7.4 s |
|---|
Radioactive decay series
- Osmium-170 7.4 s
- Rhenium-170 9.2 s · 90.5%
- Tungsten-170 2.42 min · 90.5%
- Tantalum-170 6.76 min · 90.5%
- Hafnium-170 16.01 h · 90.5%
- Lutetium-170 2.01 d · 90.5%
- Ytterbium-170 unknown · 90.5%
- Tungsten-166 19.2 s · 9.5%
- Tantalum-166 34.4 s · 9.5%
- Hafnium-166 6.8 min · 9.5%
- Lutetium-166 2.65 min · 9.5%
- Ytterbium-166 56.7 h · 9.5%
- Thulium-166 7.70 h · 9.5%
- Erbium-166 stable · 9.5%
Rare branches (below 0.01%)
Rare branches are transformations that occur in fewer than 0.01% of decays, e.g. double beta decay or cluster emission. The nuclides they produce are practically absent from a sample, so they are hidden by default to keep the main path clear. In this series: branches - 1, nuclides - 20.
- Hafnium-162 38.7 s · 0.0033%
- Lutetium-162 1.37 min · 0.0033%
- Ytterbium-162 18.89 min · 0.0033%
- Thulium-162 21.80 min · 0.0033%
- Erbium-162 stable · 0.0033%
- Ytterbium-158 1.49 min · 2.7×10⁻⁷%
- Thulium-158 3.98 min · 2.7×10⁻⁷%
- Erbium-158 2.26 h · 2.7×10⁻⁷%
- Holmium-158 11.3 min · 2.7×10⁻⁷%
- Dysprosium-158 stable · 2.7×10⁻⁷%
- Erbium-154 3.73 min · 5.6×10⁻¹²%
- Holmium-154 11.76 min · 5.6×10⁻¹²%
- Dysprosium-154 2.8×10⁶ a · 5.6×10⁻¹²%
- Dysprosium-150 7.17 min · 2.6×10⁻¹⁴%
- Terbium-150 3.48 h · 1.8×10⁻¹⁴%
- Gadolinium-150 1.79×10⁶ a · 5.6×10⁻¹²%
- Gadolinium-146 48.27 d · 9.7×10⁻¹⁵%
- Europium-146 4.61 d · 9.7×10⁻¹⁵%
- Samarium-146 6.8×10⁷ a · 5.6×10⁻¹²%
- Neodymium-142 stable · 5.6×10⁻¹²%
How to read the simulation
Grid: each pixel is one atom of the starting isotope. When an atom decays, the pixel takes the colour of the decay product - in decay series mode the product can decay further. The moment each atom decays is random, but the probability follows from the half-life, so after one T½ about half of the atoms remain, after two - about a quarter.
Chart N(t): what percentage of the sample atoms each nuclide makes up at a given moment. The line of the starting isotope falls (by half after each T½), the lines of stable products rise, and those of short-lived ones first rise, then fall.
Chart A(t): activity, i.e. the number of decays per second (becquerel, Bq). It depends on the number of atoms and on how fast they decay: for the same number of atoms, the shorter the T½, the higher the activity.
Simulation time runs faster (or slower) than real time - the time scale slider sets the multiplier. This way you can watch the decay of isotopes that live from fractions of a second to billions of years.
Well-known isotopes
- H-3 - Tritium - glowing watch hands, nuclear fusion fuel.
- C-14 - Radiocarbon dating.
- K-40 - Natural radioactivity - in bananas and in our bodies.
- Co-60 - Radiotherapy and radiation sterilization.
- I-131 - Thyroid treatment; Chernobyl fallout.
- Cs-137 - Long-lasting contamination after Chernobyl and Fukushima.
- Rn-222 - Radon in basements and mines.
- Ra-226 - The longest-lived isotope of radium - the element discovered by Marie and Pierre Curie in 1898.
- U-235 - Nuclear power plant fuel; start of the actinium series.
- U-238 - Age of the Earth; start of the uranium series.
- Pu-238 - Power source for space probes (Voyager, Curiosity rover).
- Am-241 - Ionization smoke detectors.
Data sources
- NNDC Wallet Cards 2023 - Data as of 15 October 2024 - licence: Public domain