Kilocurie to Nanocurie

In 1987, scrap metal scavengers in Goiânia, Brazil broke open an abandoned caesium-137 teletherapy source containing about 1,375 Ci (50.9 TBq). The glowing blue Cs-137 powder fascinated locals — they rubbed it on skin, gave it to children, and spread it across multiple homes. Four people died, 249 were contaminated, and the cleanup produced 3,500 m³ of radioactive waste. The incident became the textbook case for why sealed sources must be tracked and securely stored throughout their entire lifecycle, and why the IAEA created its Code of Conduct on the Safety and Security of Radioactive Sources.

Yes, multiple times. In Ciudad Juárez, Mexico (1983), a stolen Co-60 teletherapy source was sold as scrap and melted into rebar, contaminating 4,000 tonnes of steel and exposing thousands. In Samut Prakan, Thailand (2000), a junked Co-60 source killed three scrap workers who pried it open. In Yanango, Peru (1999), a welder pocketed an Ir-192 industrial radiography source and carried it in his pocket for hours — his leg was amputated. The IAEA documents over 30 serious radiation accidents involving orphaned or stolen sources since the 1960s, collectively killing dozens and injuring hundreds.

Cobalt-60 has a 5.27-year half-life, so a 500 kCi source drops to 250 kCi after five years and becomes too weak for industrial throughput after about 15–20 years. The spent source pencils are returned to the manufacturer (typically in Canada or Russia) for reprocessing or secure storage. Transport uses heavily shielded Type B casks certified to survive a 9-meter drop and 30-minute fire. The manufacturer often offers a swap program: deliver fresh sources and take back decayed ones in the same shipment, minimising the number of high-activity transports.

The Fukushima Daiichi disaster released an estimated 10–30 PBq (10,000–30,000 TBq) of caesium-137 directly into the Pacific Ocean between March and July 2011 — the largest single marine radioactive release in history. For comparison, the Sellafield reprocessing plant in the UK discharged about 40 PBq of Cs-137 into the Irish Sea over decades of operation (1952–2000). Soviet dumping of entire reactor compartments from nuclear submarines in the Arctic added further inventory. Despite these numbers, ocean dilution is vast: Pacific Cs-137 levels from Fukushima peaked at about 50 Bq/m³ near the plant and dropped below 2 Bq/m³ within a few hundred kilometers.

This is exactly why the IAEA, NRC, and national agencies track high-activity sources so aggressively. A kilocurie Cs-137 or Co-60 source dispersed by conventional explosives would contaminate a few city blocks — not causing acute radiation casualties (the blast itself is deadlier) but creating a costly, panic-inducing cleanup lasting months. The actual health risk to the public would be low, but the economic and psychological damage would be enormous. Post-9/11 programs like the US GTRI (now NNSA OSRP) have recovered or secured thousands of orphaned high-activity sources worldwide.

Receptor binding assays are the classic example. A biochemist adds 2–5 nCi of tritium-labelled drug to a plate of cells and measures how much binds to a receptor versus washing away. Metabolic tracing studies use similar amounts of carbon-14-labelled glucose or amino acids to follow biochemical pathways. At nanocurie levels the radioactivity is low enough that bench work requires minimal shielding — a few centimeters of acrylic for tritium beta particles — but high enough to produce a detectable signal after hours of counting.

One nanocurie equals 37 Bq — about the activity of 2.5 bananas worth of potassium-40, or roughly 0.5% of the natural K-40 activity in your own body. A smoke detector contains about 30,000 nCi (1 µCi) of americium. The nanocurie sits in the gap between environmental levels you cannot avoid (picocuries) and laboratory quantities that require formal licensing (microcuries). It is the unit of "detectable but not dangerous," which is exactly why it suits low-level lab work.

Tritium (hydrogen-3) is the perfect biological tracer because hydrogen appears in every organic molecule. You can replace a hydrogen atom with tritium without changing the molecule's chemistry — the drug, amino acid, or sugar behaves identically in the cell. Tritium emits only very low-energy beta particles (max 18.6 keV) that cannot penetrate skin or even a lab bench surface, making it the safest radioisotope to handle. The downside is low specific activity, so you need sensitive liquid scintillation counting to detect it — but at nanocurie levels, that is perfectly adequate.

In the US, NRC exempt quantities vary by isotope. For tritium, the exempt quantity is 1,000 µCi (1 mCi); for carbon-14 it is 100 µCi; for iodine-125 it is just 1 µCi. Nanocurie-scale quantities are generally below exempt limits for most isotopes, but universities and companies typically hold broad licenses covering all their work anyway. The license requirements are not about the activity alone — they are about accountability, training, waste disposal, and ensuring that small amounts do not accumulate into large ones through careless stockpiling.

For short-lived isotopes (half-life under 120 days), most institutions use "decay in storage" — the waste sits in a shielded cabinet for 10 half-lives until it is indistinguishable from background, then gets disposed of as normal chemical waste with all radioactive labels removed. For longer-lived isotopes like tritium (12.3-year half-life) or carbon-14 (5,730 years), the waste is collected in designated containers, catalogd by isotope and activity, and shipped to a licensed low-level radioactive waste broker. At nanocurie levels the volumes are small, so the main cost is paperwork, not shielding.