The Linear No Threshold model (Howard Hayden) USofA

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The Energy Advocate August 2016 (Vol. 21, No. 1)

A monthly newsletter promoting energy and technology P.O. Box 7609, Pueblo West, CO 81007 Copyright © The Energy Advocate

The LNT The Linear-No-Threshold (LNT) model is commonly used by the Nuclear Regulatory Commission (NRC) to predict possible outcomes of radiation exposures. Specifically, it says that the likelihood of a cancer resulting from exposure is directly proportional to the amount of exposure (the dose). To be specific, the model says that the straight line in the graph extends all the way down to the 0 zero-dose, zero-response point 0 (0,0). The contentious part of the LNT is about the response at very low doses: are very low doses actually hazardous? It is often easy to infer doses accurately, so the position on the horizontal axis can be accurately determined. Only for very strong doses can you determine the hazard, and even that is not so easy. For example, in the bombings of Hiroshima and Nagasaki, there were something like 100,000 survivors who received near-fatal doses, yet it took sophisticated statistical techniques to find that a few hundred cancers resulted from the radiation, against a background of about 20,000 cancers that would have happened anyway. We will show below that the measure of radiation dose is not an additive quantity. It follows that the response (such as cancer) is not necessarily proportional to dose. That much said, what is the importance of the possible offset from the (0,0) point? It is simply this: the population of the US is about 300 million, and of the world is about 7 billion. If you assume that some minuscule radiation exposure to the population will cause a cancer in one person in 1,000,000 people, then there will be 300 cancers in the US and 7,000 cancers in the world. Never mind that there are already over 590,000 annual deaths due to cancer in the US. The 300 presumed deaths add to it, and our regulators get upset about that, and impose stringent, expensive rules on the nuclear industry (and the health industry as well) to be careful. If the dose-response curve shows a threshold—that is, a dose below which there is no harmful response—then the

Radiation Exposure When we talk about radiation, we are usually talking about three kinds, dubbed alpha (), beta () and gamma (), by early scientists who did not know at the time exactly what the radiation was all about. It was soon learned that -particles are the nuclei of helium atoms, ejected from some nuclei such as radium and uranium. (They were identified as such by deflection in magnetic fields, and proved as such by the presence of helium atoms above a mercury column in which radium had been introduced.)

stringent rules become unnecessary. Nuclear power becomes, perforce, cheaper. Another dose-response curve is the hormesis model, in which the response on the graph is LT Model negative. That is, a small dose is beneficial instead of harmful. In this case the stringent rules are not only expensive, but actually harmful. For example, in Fukushima, there were over 1,000 evacuation-related deaths to escape radiation doses that were far below levels naturally occurring elsewhere. Japan decided to shut off all nuclear reactors and get the electricity from more-polluting, imported high-cost fuels. And what if a small dose of radiation actually reduces cancer incidence instead of causing more cancer? Another consideration is whether the high costs imposed by overregulation cause some early deaths, say, by poverty. A recent letter to Physics Today [1] made a case for the threshold model: Muller’s and Stern’s approaches survive in the LNT model of today, which says that low-dose radiation increases cancer risk. However, while linearity—the “L” in LNT—was demonstrated only at high doses, the absence of a threshold has never been demonstrated. The only scientific conclusion from the data from 1949 through today is that the linear threshold (LT) model, not the LNT, is correct, and it has a lowdose threshold below which radiation is harmless. Even data from atomic-bomb survivors, the gold standard of doseresponse data, do not support the LNT model; adaptive protections mitigate radiation-induced damage at low doses and low dose rates. No epidemiological studies have ever demonstrated a causal relationship between low-dose radiation exposure and carcinogenesis.

Some letters in the subsequent edition [2] of Physics Today insisted that the LNT is correct, and others insisted that it is not correct. [1]

Jeffry A. Siegel, Charles W. Pennington, and Bill Sacks, “Lowdose radiation exposure should not be feared,” Physics Today 69(1), 12 (2016); online at http://dx.doi.org/10.1063/PT.3.3037

[2]

J. S. Levinger, “The linear no-threshold theory: Readers weigh in,” Physics Today 69(7), 10 (2016); online at http://dx.doi.org/10.1063/PT.3.3037

Beta () particles are nothing but ordinary electrons that are ejected by some nuclei when one of the neutrons breaks apart into a proton (which remains in the nucleus) and the escaping electron. Gammas () are electromagnetic radiation—like ordinary light—but of much higher energy, emitted along with  and  emissions. X-rays, also electromagnetic radiation, are created by colliding high-energy electrons with metals (often tungsten). Cosmic rays in space are mostly high-energy protons, but they result in high-energy x-rays caused by collisions with atmospheric gases.


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