MICROWAVE DIATHERMY TREATMENT OF THE HUMAN THIGH PART I The Experimental Measurement of the Muscle Blood Flow in the Thigh Undergoing Microwave Diathermy Treatment
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915 MHz microwaves caused 16-fold increases in human muscle blood flow, proving significant biological effects from frequencies used in wireless technology.
Plain English Summary
Researchers used 915 MHz microwave diathermy on healthy volunteers' thigh muscles while measuring blood flow at different depths. They found blood flow increased dramatically from 2 to 32 ml/min/100g, with deeper muscle tissue showing different response patterns than surface tissue. This demonstrates how microwave energy penetrates and affects human tissue circulation.
Why This Matters
This therapeutic study reveals something crucial about microwave radiation and human biology: 915 MHz microwaves don't just heat tissue surface-level, they penetrate deep enough to trigger significant physiological changes in muscle blood flow. The 16-fold increase in circulation demonstrates the body's vascular system responding dramatically to microwave exposure. What makes this particularly relevant is that 915 MHz sits right in the range of many wireless technologies we use daily. While this was therapeutic diathermy with direct skin contact, it shows how readily human tissue responds to microwave frequencies. The researchers needed surface cooling to prevent overheating at the fat-muscle interface, highlighting how efficiently these frequencies transfer energy into our bodies. The different blood flow patterns at 1.5 cm versus 3.0 cm depth prove that microwave effects aren't uniform throughout tissue layers.
Exposure Information
Specific exposure levels were not quantified in this study.
Show BibTeX
@article{microwave_diathermy_treatment_of_the_human_thigh_part_i_the_experimental_measure_g5359,
author = {redacted},
title = {MICROWAVE DIATHERMY TREATMENT OF THE HUMAN THIGH PART I The Experimental Measurement of the Muscle Blood Flow in the Thigh Undergoing Microwave Diathermy Treatment},
year = {n.d.},
}