{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,12]],"date-time":"2026-09-12T10:34:26Z","timestamp":1789209266977,"version":"build-2803163510"},"reference-count":14,"publisher":"Wiley","issue":"1","license":[{"start":{"date-parts":[[2005,10,19]],"date-time":"2005-10-19T00:00:00Z","timestamp":1129680000000},"content-version":"vor","delay-in-days":7596,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Bioelectromagnetics"],"published-print":{"date-parts":[[1985,1]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>Further studies of human whole\u2010body radiofrequency (RF) absorption rates were carried out using a TEM\u2010cell exposure system. Experiments were done at one frequency near the grounded resonance frequency ( \u223c 40 MHz), and at several below\u2010resonance frequencies. Absorption rates are small for the K and H orientations of the body, even when grounded. For the body trunk in an E orientation, the absorption rate of a sitting person is about half of the rate for the same person standing with arms at the sides; the latter in turn is about half the rate for the same subject standing with arms over the head. Two\u2010body interactions cause no increase in absorption rates for grounded people. They do, however, increase the absorption rates for subjects in an E orientation in free space; the largest interaction occurs when one subject is \u03bb\/2 behind the other (as seen by the incident wave). When these results are applied to practical occupational exposure situations, the whole\u2010body specific absorption rate does not exceed the ANSI limit of 0.4 W\/kg for exposures permitted by the ANSI standard (C95.1\u20101982) at frequencies from 7 to 40 MHz.<\/jats:p>","DOI":"10.1002\/bem.2250060104","type":"journal-article","created":{"date-parts":[[2006,2,4]],"date-time":"2006-02-04T00:25:24Z","timestamp":1139012724000},"page":"33-40","source":"Crossref","is-referenced-by-count":16,"title":["Further studies of human whole\u2010body radiofrequency absorption rates"],"prefix":"10.1002","volume":"6","author":[{"given":"Douglas A.","family":"Hill","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"311","published-online":{"date-parts":[[2005,10,19]]},"reference":[{"key":"e_1_2_1_2_1","unstructured":"ANSI(1982): ANSI C95.1\u20101982 American national standard\u2014safety levels with respect to human exposure to radio\u2010frequency electromagnetic fields 300 kHz\u2010100 GHz."},{"key":"e_1_2_1_3_1","doi-asserted-by":"publisher","DOI":"10.1109\/TMTT.1977.1129206"},{"key":"e_1_2_1_4_1","unstructured":"DurneyCH JohnsonCC BarberPW MassoudiH IskanderMF LordsJL RyserDK AllenSJ MitchellJC(1978): \u201cRadio\u2010frequency Radiation Dosimetry Handbook \u201d Ed. 2. Report SAM\u2010TR\u201078\u201022 USAF School of Aerospace Medicine Brooks AFB Texas. Springfield Virginia: NTIS."},{"key":"e_1_2_1_5_1","doi-asserted-by":"publisher","DOI":"10.1029\/RS014i06Sp00015"},{"key":"e_1_2_1_6_1","unstructured":"GuyAW ChouC\u2010K(1982): Hazard analysis: Very low frequency through medium frequency range. Final Report USAF SAM contract 33615\u201078\u2010D\u20100617. Dept of Rehab Medicine University of Washington Seattle WA 98195."},{"key":"e_1_2_1_7_1","doi-asserted-by":"publisher","DOI":"10.1109\/TMTT.1982.1131333"},{"key":"e_1_2_1_8_1","doi-asserted-by":"publisher","DOI":"10.1080\/16070658.1983.11689323"},{"key":"e_1_2_1_9_1","doi-asserted-by":"publisher","DOI":"10.1002\/bem.2250050203"},{"key":"e_1_2_1_10_1","doi-asserted-by":"publisher","DOI":"10.1109\/TMTT.1984.1132771"},{"issue":"1","key":"e_1_2_1_11_1","article-title":"Better simple models of human radiofrequency absorption rates for E polarization at quasi\u2010static frequencies","volume":"20","author":"Hill DA","year":"1985","journal-title":"J Microwave Power"},{"key":"e_1_2_1_12_1","doi-asserted-by":"crossref","first-page":"325","DOI":"10.1080\/16070658.1983.11689338","article-title":"Resonance suppression in a TEM cell","volume":"18","author":"Hill DA","year":"1983","journal-title":"J Microwave Power"},{"key":"e_1_2_1_13_1","unstructured":"HillDA WalshJA(1984): The effect of wave impedance on human whole\u2010body radio\u2010frequency absorption rates. Report No. 891 Defence Research Establishment Ottawa 1984."},{"key":"e_1_2_1_14_1","doi-asserted-by":"crossref","unstructured":"HillDA WalshJA(1985): Radio\u2010frequency current through the feet of a grounded human. IEEE Trans Electromagn Compat in press.","DOI":"10.1109\/TEMC.1985.304241"},{"key":"e_1_2_1_15_1","doi-asserted-by":"publisher","DOI":"10.1029\/RS012i06Sp00065"}],"container-title":["Bioelectromagnetics"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/api.wiley.com\/onlinelibrary\/tdm\/v1\/articles\/10.1002%2Fbem.2250060104","content-type":"unspecified","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/pdf\/10.1002\/bem.2250060104","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2023,10,21]],"date-time":"2023-10-21T12:54:12Z","timestamp":1697892852000},"score":1,"resource":{"primary":{"URL":"https:\/\/onlinelibrary.wiley.com\/doi\/10.1002\/bem.2250060104"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[1985,1]]},"references-count":14,"journal-issue":{"issue":"1","published-print":{"date-parts":[[1985,1]]}},"alternative-id":["10.1002\/bem.2250060104"],"URL":"https:\/\/doi.org\/10.1002\/bem.2250060104","archive":["Portico"],"relation":{},"ISSN":["0197-8462","1521-186X"],"issn-type":[{"value":"0197-8462","type":"print"},{"value":"1521-186X","type":"electronic"}],"subject":[],"published":{"date-parts":[[1985,1]]}}}