Bahareh Behzadnezhad1,2, Jian Dong1, Nader Behdad1, and Alan McMillan2
1Dept of Electrical and Computer Engineering, University of Wisconsin-Madison, Madison, WI, United States, 2Dept of Radiology, University of Wisconsin-Madison, Madison, WI, United States
Synopsis
This study describes a very low-cost EPR spectrometer
that can be feasibly constructed using general purpose laboratory equipment
combined with the use of 3D electromagnetic design and additive manufacturing.
We demonstrate a functioning, homebuilt, low-cost continuous wave EPR
spectrometer operating at 115 MHz. The development of a low-cost spectrometer has
applications in education and for other general laboratory purposes.
Purpose
The purpose of
this study is to demonstrate that a low-cost EPR spectrometer can be
constructed by leveraging additive manufacturing to build various system
components. Herein, we demonstrate a homebuilt, low-cost continuous wave (CW) EPR
spectrometer operating at 115 MHz where the structure of electromagnetic
components (modulation coils and resonator) have been constructed using additive
manufacturing (3D printing).Methods
The block diagram of the constructed CW EPR
spectrometer is shown in Figure 1. Components of the spectrometer can be
divided into three categories: (1) Electromagnetic Components including the main
electromagnet, modulation coil, and radio frequency (RF) resonator, (2) RF bridge,
and (3) Data acquisition system. (1)
The main magnet was wound with a single layer of 140 turns of #12 copper wire on
a 30-cm polycarbonate tube. The electromagnet provides 4.1 mT magnetic field (corresponding
to a 115 MHz EPR frequency) at 15 amps using a DC programmable power supply (XFR
150-18, AMETEK, San Diego, CA). The modulation field is generated with a
Helmholtz coil (coil diameter of 11 cm) for which the frame was constructed
using additive manufacturing from ABS plastic filament on an available 3D
printer (Creator X, Flashforge, Rowland Heights, CA). The modulation coil was
driven by an audio-frequency amplifier. The RF resonator uses a parallel loop
configuration in conjunction with a capacitive impedance matching network similar
to designs previously utilized for EPR spectroscopy/imaging1. Full-wave
electromagnetic simulations in CST Studio (Darmstadt, Germany) were used to
design and simulate the parallel loop structure, including the material
properties (e.g., dielectric loss, thermal, and mechanical properties) of all
resonator components. The mechanical design of loop’s supporting structure was
then 3D printed in ABS plastic. The simulated scattering parameter
(S-parameters) of the loop were then exported into electronic design software ADS
(Keysight Technologies, Santa Rosa, CA) to design and optimize the resonator as
well as to determine component values of the capacitive impedance matching
network. Figure 2 shows the simulated and fabricated parallel loop resonator
and the modulation coil. Figure 3 shows the measured reflection coefficient (S11)
of the resonator. (2) The RF bridge
(shown in Figure 4) is a homodyne reflection-type bridge using a double
balanced mixer as detector to ensure that signal phase information can be
accurately measured. A 180° hybrid coupler was used to direct signal to and
from the resonator and provide 40 dB decoupling between source and detector. A 16dB
attenuator was used in the reference arm and the required phase shift was attained
by adjusting the cable length. A signal generator (AFG 3251, Tektronix,
Beaverton, OR) was used as the main RF source. (3) Data acquisition is based on a commercially available lock-in
amplifier (AMETEK 7230) connected to a PC via an Ethernet connection. Custom
software written in MATLAB (The Mathworks, Natick, MA) was used to control the
lock-in amplifier. The oscillator of the lock-in amplifier was used to generate
the modulation signal (at 20 kHz, chosen based on the phase noise measurements
of the RF source). An auxiliary digital-to-analog (DAC) signal from the lock-in
amplifier was used to control the field sweep of the main magnet. To evaluate
the prototype spectrometer, a sample of DPPH powder (D9132, Sigma Aldrich) was
placed in the resonator and the EPR spectra was measured at a transmit power of
10 dBm.Results
Figure 5 shows the measured EPR spectrum of DPPH
in the prototype spectrometer using 100 points and averaging. Measurements were
performed using a B0 field sweep between 3 to 5.5 mT and the total
measurement time was approximately 5 minutes. Discussion and Conclusion
This abstract
demonstrates the design and construction of a low-cost, homebuilt EPR
spectrometer. Such a system can be designed and implemented quickly with very
low cost for educational or general laboratory purposes. When existing general
purpose laboratory equipment can be utilized (e.g., DC power supply, signal
generator, lock-in amplifier, 3D printer), the remaining costs of constructing
an operating EPR spectrometer can be very low (less than $2,500 USD for the
system presented here). The entire process is enhanced by the use of 3D design,
where the mechanical structure of components can be designed and subsequently imported
into EM simulation software to perform rapid design iteration of highly
optimized electromagnetic components prior to construction. Additive
manufacturing provides a low-cost and rapid means to construct these components.
Future work includes the development of the spectrometer at higher B0 field
strengths as well application of the 3D design and additive manufacturing
techniques to construct gradient coils to extend the device to imaging.Acknowledgements
The project described was supported by the Clinical and Translational Science Award (CTSA) program, through the NIH National Center for Advancing Translational Sciences (NCATS), grant UL1TR000427. The content is solely the responsibility of the authors and does not necessarily represent the official views of the NIH.References
1- Devasahayam,
N., et al. "Parallel coil resonators for time-domain radiofrequency
electron paramagnetic resonance imaging of biological objects." Journal of
Magnetic Resonance 142.1 (2000): 168-176.