The purpose of this work is to develop a simple reference standard to be used for gradient-induced heating tests to verify test system operation. A second objective is to provide data on measurement repeatability of heating in these reference objects. Two different dB/dt exposures (270 Hz and 1000 Hz) were used to measure the gradient-induced temperature rise of three MRI compatible metals using a laboratory dB/dt exposure system. Based on the temperature rise, an MRI compatible metal of distinct dimensions and geometry was determined to be most suitable as a dB/dt heating standard across a frequency range of 270-1000 Hz.
The gelled hydroxyethyl cellulose (HEC) phantom material was prepared in accordance with [2], consisting of 31 g/L HEC powder and 1.52 g/L NaCl in distilled water. The gelled HEC serves to simulate human tissue, sharing similar conductive and thermal properties, alongside limiting internal conduction and minimalizing thermal convection. Four copper annuli, two stainless-steel annuli, and two titanium annuli were measured for temperature change when subjected to gradient field exposure. All annuli had a 5-cm outer diameter with varying thickness and varying inner diameters. A water-cooled solenoid electromagnet, an amplifier (Copley Controls Corp., Model 266), and a waveform generator were integrated into a dB/dt exposure system and used to produce gradient dB/dt field exposures as specified in Clause 9 of ISO 10974 [3]. Two different dB/dt exposures were used: a continuous 270 Hz sinusoidal wave (dB/dt value of 42 T/s rms), and a continuous 1000 Hz sinusoidal wave (dB/dt value of 42 T/s).
Temperature was measured by two fiber optic temperature probes (Neoptix Inc., T1C-15548A) placed in 1-mm holes on the outer edges of each annuli. The metal annuli were centered in a phantom with a 13-cm diameter and a 9-cm gel height. The metal annuli underwent three repeated exposures, each involving a 20-second gradient exposure followed by 160-seconds of cool-down time. Two fiber optic probes collected temperature readings of the annulus during each trial, totaling six temperature readings per three trials for each condition. A third probe was placed in the gelled HEC ensuring the media did not significantly heat up and lose its thermal properties. A fourth probe was placed on the boundary surrounding the gradient coil measuring the ambient temperature, ensuring tests were being conducted in a stable environment.
Boxplots summarizing temperature change for all copper annuli at 270 Hz over 5 sessions (i.e., 15 trials, i.e., 30 temperature readings)
Boxplots summarizing temperature change for all copper annuli at 1000 Hz (1 kHz) over 2 sessions (i.e., 6 trials, i.e., 12 temperature readings)