Dielectric Properties of the Human Body for Wave-lengths in the 1-10 cm. Range
T. S. England · 1950
This 1950 study established foundational science on how microwave radiation interacts with human tissues at frequencies now used by modern wireless devices.
Plain English Summary
This 1950 study measured how microwave radiation at three different wavelengths (1.27 cm, 3.18 cm, and 10 cm) interacts with human body tissues taken from surgical operations. Researchers analyzed the dielectric properties of various tissues to understand how microwaves penetrate and affect different parts of the human body. This foundational research helped establish how electromagnetic fields interact with biological tissues.
Why This Matters
This pioneering 1950 research represents some of the earliest scientific investigation into how microwave radiation interacts with human tissue - work that laid the groundwork for understanding EMF bioeffects decades before cell phones existed. The study's focus on wavelengths between 1-10 cm is particularly relevant today, as these frequencies overlap with modern wireless technologies including WiFi, Bluetooth, and cellular communications. What makes this research significant is that it established the basic science of how electromagnetic fields penetrate biological tissues, showing that different body tissues have varying electrical properties that affect EMF absorption. The reality is that this fundamental research on tissue dielectric properties directly informs modern specific absorption rate (SAR) calculations used to supposedly 'protect' us from wireless radiation - yet these safety standards were developed primarily from this type of basic physics research, not comprehensive health studies.
Exposure Information
Specific exposure levels were not quantified in this study.
Show BibTeX
@article{dielectric_properties_of_the_human_body_for_wave_lengths_in_the_1_10_cm_range_g3936,
author = {T. S. England},
title = {Dielectric Properties of the Human Body for Wave-lengths in the 1-10 cm. Range},
year = {1950},
}