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0 ' BNL-63574 BEC 2 3 19% The Linear, No-treshold Hypothesis Lin &&th Effects to Tissue Absorbed Dose Appears Principally Inapplicable at Low Doses. 1 Ludwig E. Feinendegenl, Victor P. Bond', Charles A. Sondhaus2. ' 'Medical Department, Brookhaven National Laboratory, Upton, N.Y. 'Radiation Control Office, University of Arizona, Tucson, A.Z. Introduction: The probability of detrimental effects (R), such as cancer induction in irradiated multicellular tissue, from low- dose exposure to ionizing radiation is conventionally related to absorbed dose (D)" to tissue by the proportionality constant cc for a given type of radiation: R = a -D. This expression formalizes the linear no-treshold hypothesis stating that radiation exposure may be harmful at all dose levels. The present paper challenges the validity of this hypothesis by examining tissue re.sponses as an integral consequence of multiple and various cell responses especially at low dose levels. T Description of the actual work: According to microdosimetry (18) , tissue absorbed dose D is equal to the product of zl and NH/N,, with zl denoting the frequency-averaged specific energy deposited in a defined mass of microscopic dimension such as a cell (hit- size or cell dose), and NJN, being the number of hits of any size within the number of exposed cells of that mass:

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  • 0 '

    BNL-63574

    BEC 2 3 19%

    The Linear, No-treshold Hypothesis Lin &&th Effects to Tissue Absorbed Dose Appears Principally Inapplicable at Low Doses.

    1

    Ludwig E. Feinendegenl, Victor P. Bond', Charles A. Sondhaus2. '

    'Medical Department, Brookhaven National Laboratory, Upton, N.Y. 'Radiation Control Office, University of Arizona, Tucson, A.Z.

    Introduct ion: The probability of detrimental effects (R), such as

    cancer induction in irradiated multicellular tissue, from low-

    dose exposure to ionizing radiation is conventionally related to

    absorbed dose ( D ) " to tissue by the proportionality constant cc

    for a given type of radiation:

    R = a - D .

    This expression formalizes the linear no-treshold hypothesis

    stating that radiation exposure may be harmful at all dose

    levels. The present paper challenges the validity of this

    hypothesis by examining tissue re.sponses as an integral

    consequence of multiple and various cell responses especially at

    low dose levels. T Description of the actual work: According to microdosimetry (18) , tissue absorbed dose D is equal to the product of zl and NH/N,, with zl denoting the frequency-averaged specific energy deposited in a defined mass of microscopic dimension such as a cell (hit-

    size or cell dose), and NJN, being the number of hits of any

    size within the number of exposed cells of that mass:

  • D=Cl *N,/Ne.

    2

    The mass of the average cell in mammalian tissue is taken to be 1

    ng

    events, hits, that are caused by discrete ionizing subatomic

    particles traversing, or being confined to, cells. The value of

    cl is a constant for a given type of radiation. The conventional dose-risk-function, R = a D, is then transformed into the

    cellular hit-number-effectiveness-function:

    9 * 13# ". Cell doses derive from single energy deposition

    with Nq being the number of malignant tumors in the exposed cells 2 Ne

    Much data are available on single cell responses to hits from

    ionizing radiation both from own work 7 r lo# l4, 16, 33 and that of

    . Estimates of the probabilities of others 6, 19, 22, 24, 25, 26, 27, 28, 32 various cellul'ar responses and of their individual changes with

    N,, are used to describe the term ar as the sum of these

    probabilities with positive and negative terms 14, 15.

    Results: Malignant tumors have been observed to arise from single

    cells. Within the dose range where observable incidences of

    detriment such as malignant transformation of cells are

    proportional to the value of tissue absorbed dose 29, individual

  • DISCLAIMER

    . This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or use- fulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any spe- cific commercial product, proctss, or service by trade name, trademark, manufac- turer, or otherwise does not necessarily constitute or imply its endorsement, recom- mendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.

  • DISCLAIMER

    Portions of this document may be illegible in electronic image products. Images are produced from the best available original document.

  • 3

    hits are assumed to act independently of each other in causing

    detriment in the exposed cells. In case of a supra-linear

    response, individual hits are assumed to have the probability of

    enhancing the capability of single hits to cause the development

    of a malignant tumor.

    However, within complex multicellular tissue, hit cells also

    respond acutely and temporarily by a variety of biochemical

    reactions that potentially confer protection against the

    accumulation of DNA damage in tissue. This is irrespective of the

    cause of that damage. Since DNA damage has been related to the

    development of cancer ‘I, ?I, protection against DNA damage in

    tissue is assumed to also operate against the development of

    cancer.

    The protective or adaptive cellular responses to low doses ’t 21t 24

    are likely triggered by a sudden change in the intracellular

    concentration of free radical molecules produced by hits on cells

    8 e lo. These responses appear temporarily over various periods of

    time ranging from hours to days, and include the following

    categories: 1. stimulation of the cellular radical detoxification

    system with prevention of attacks by radicals on cellular

    constitutent molecules 8 r l o t 16; 2. stimulation of cellular

    mechanisms that reduce DNA-damage possibly through repair 2 4 t 2 5 r 2 6 v

    32; 3 . induction of programmed cell death, called apoptosis 19; 4.

    induction of the immune system recognizing and eliminating cells

  • 4

    that carry malignant transformation 2 2 . Each of these adaptive

    responses appears to have its own probability 3r 12# 14#

    all act towards preventing and/or reducing lasting DNA damage in

    the exposed tissue. Clastogenic factors must also be considered

    to initiate adaptive responses. The probability of protection

    against action of radicals and of reduction of DNA damage per hit

    has been shown in various cell systems to decrease with tissue

    doses extending above 0.1 Gy and is seen in one system (mouse

    bone marrow) to have a maximum at a tissue dose of between 0.1

    and 0.2 Gy of low LET radiation 14# 2 7 .

    2 8 . They

    Thus, individual cells when exposed to ionizing radiation are

    taken to have different probabilities of a malignant

    transformation with the consequence of cancer:

    Pspo = spontaneous malignant

    transformation,

    Pind = radiation induced malignant

    transformation per average hit,

    penh = enhancement of Pind per average hit,

    pprot = protection against DNA damage in

    surviving cells per average hit,

  • P

    5

    The probability of cancer induction per hit can then be written

    as:

    - With Nq/NH = a Z1 (see equation 3)

    For low-LET"radiation, Pqnh is taken to be zero. Since the

    negative term in a, ppcot (pspo t pind ) , but not the positive term

    pi,,d (1 t Psnh)l is shown to be potentially an inverse function of

    N, at low doses of low-LET radiation, a can not be accepted being

    principally constant at low doses of low-LET radiation 12* 1 4 # 15.

    With pin,, for hemopoietic stem cells being about for human

    leukemia 1.21 with pel,,, being considered zero for low-LET radiation,

    and with pspo for the same cell type having been estimated to be

    about 1 4 / the value of the negative term of pprot (pspo t Pind )

    in a would become equal to Pind (1 t P&) if pprot is at low-

    level exposure to low-LET radiation. In this case, there would be

    a threshold for R developing with increasing D. In fact, many

    epidemiological and experimental data 2 o r

    existence of a threshold or even beneficial, hormetic, effects at

    low doses from low-LET radiation.

    3o support the

  • 6

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  • 7

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  • 8

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    Acknowledgement : The authors greatly appreciate the critical comments and discussion by Prof. D. Harder, Georg-August University of Goettingen, Germany. and the critical review of the mathematical prsentation in the manuscript by Dr. W. Simon, University of Rochester Medical Center, N.Y.

    This research was supported in part by the United States Department of Energy under Contract No. DE-AC02-76CH00016.