Tomoya Kimura1, Atsushi Shiina1, Kenji Takahashi2, and Kagayaki Kuroda1,3
1Course of Electrical and Electronic Engineering, Graduate School of Engineering, Tokai University, Hiratsuka, Japan, 2Department of Orthopaedic Surgery, Nippon Medical School, Tokyo, Japan, 3Center for Frontier Medical Engineering, Chiba University, Chiba, Japan
Synopsis
Temperature
dependence of T1 of tissue water in the porcine knee joint cartilage in vitro was
examined at 9.4T in comparison with that of the water proton resonance
frequency. The absolute value of T1 at each temperature between room
temperature and 60oC was reproducible. Hysteresis was negligible during heating
and cooling processes. The correlation coefficient with temperature was higher
than 0.998, and hence that with water proton chemical shift was also high
(>= 0.996). The temperature coefficient was 1.28%/oC at 30oC for heating and
1.24%/oC for cooling. These results suggested that T1 is a favorable index for
thermometry of the knee joint cartilage under thermal therapies.
Introduction
Thermal
therapy for osteoarthritis is becoming one of the options for pain-relief(1). In
order to optimize the therapeutic effect, temperature visualization of the cartilage
is indispensable, but rarely investigated to date. We have demonsrated the feasibility
of noninvasive temperature imaging of knee joint cartilage under thermal therapy
using water proton resonance freqrequency shift measured as phase shift(2).
This technique is, however, useful only when the knee joint position and
posture are unchanged during heating. The phase shift measument is suffered not
only by the object displacement itself but also by the static magnetic field
change due to the object displacement. When entire knee joint is heated like in
warm bath treatment or kinesiologic approach, referenceless type of techniues
(3, 4) based on interpolation of phase field is not applicable. In order to
find a technique to measure temperature without an image subtraction, we have considered
the use of spin-lattice relaxation time, T1, for mesuring absolute temperature
of the knee joint cartilage. As a feasibility study, we have examined the
temperature dependence of T1 in the knee joint cartilage in vitro in comparison
with that of the water proton resonance frequency.
Methods
Proton spectra of cartilage segment samples collected
from porcine knee joints were observed in a 9.4 T NMR spectrometer. The sample
was immersed in deuterium oxide (D
2O, 99%, Sigma-Aldrich) in a NMR
sample tube of 5 mm in diameter. Trimethylsilyl propanoic acid (TSP) was added
as an internal reference. After turning off auto field-frequency locking and
shimming systems, the proton spectra were evaluated at various temperature ranging
from room temperature, 30, 40, 50 and 60
oC. The sample temperature
was controlled with an air blower system equipped with the spectrometer. Then a
conventional inversion recovery sequence with the following conditions yielded
T1 of water proton in the sample; TR, 30 s; TI, 0.1, 0.2, 0.4, 1.0, 2.0. 4.0,
8.0, and 16 s, observation bandwidth, 8.012 kHz, and number of spectral points,
65536. The area of water peak was obtained over 4ppm around the center
frequency at each temperature, and used for T1 calculation.
Results
The spectrum of the cartilage sample exhibited a water
signal with negligible (0.02-0.03 %) fractions of the other components as shown
in Fig. 1. Thus the water proton resonance frequency as well as the peak area
of the water signal was readily measured from the spectrum. The relationship
between temperature and T1 in six independent measurements is plotted in Fig.
2a, while that between temperature and the water proton chemical shift measured
from TSP is in Fig. 2b. The temperature coefficient of the water proton T1 was
36.9 ms/
oC (1.28%/
oC at 30
oC) for heating period and 36.0 ms/
oC
(1.24%/
oC at 30
oC) for cooling. The two temperature coefficient did not have
significant difference, and thus no hysteresis was recognized in the
temperature range used in the present study. The correlation between the two
temperature indicators is also plotted in Fig. 3, showing that the correlation
was higher than 0.996.
Discussion
This work was straight forward
examination to evaluate if T1 of the knee joint cartilage can be an index for
absolute temperature measurement. As is seen from Fig. 2, the temperature
dependence of the parameter is quite reproducible in a range from room
temperature to 60
oC. Because no hysteresis was recognized, tissue denaturation
seemed to have no effect on the T1 temperature dependence in this temperature
range. In the imaging scheme for the particular tissue like knee cartilage,
resonance frequency change measured with phase difference will be strongly suffered
by tissue displacement and static magnetic field change. On the other hand, T1
can be mapped as its absolute value without difference calculation, although a
quick T1 mapping method like with multiple flip angles needs care for B1 field
homogeneity. These results support that T1 is a strong candidate for measuring
absolute temperature in the cartilage, and thus temperature imaging unaffected
by the tissue displacement is greatly expected.
Conclusion
Feasibility of noninvasive and
absolute MR thermometry for knee joint cartilage based on T1 was demonstrated.
Although blood flow in the cartilage is poor and thus the in vitro results
shown here should be valid in the in vivo tissues, similar careful study has to
be made using living animals. Rapid T1 mapping technique with multiple flip
angle approach to image the absolute temperature is under our current
examination.
Acknowledgements
This study was supported by grant-in-aid
of Ministry of Education, Culture, Sports, Science and Technology, Japan.References
(1) Takahashi K, Kurosaki H, Hashimoto S, Takenouchi K,
Kamada T, Nakamura H.The effects of radiofrequency hyperthermia on pain and
function in patients with knee osteoarthritis: a preliminary report. J Orthop
Sci. 2011 Jul;16(4):376-81.
(2) Shiina A, Takahashi K, Nakano J, Kuroda K.
Feasibility of Temperature Imaging of Knee Joint Cartilage Under Thermal
Therapy Using Water Proton Resonance Frequency Shift. Proc 23rd Annual Meeting
& Exhibition, Int Soc Magn Reson Med, Toronto 2015:p. 4057.
(3) Rieke V, Vigen KK, Sommer G, Daniel BL, Pauly JM ,
Butts K,. Referenceless PRF Shift Thermometry. Magn Reson Med 2004;51:1223-1231.
(4) Kuroda K, Kokuryo D,
Kumamoto E, Suzuki K, Matsuoka1 Y, Keserci B. Optimization of Self-reference
Thermometry using Complex Field Estimation. Magn Reson Med 2006;56(4):835-843.