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. 2017 Jun;7(3):356–368. doi: 10.21037/qims.2017.06.06

Table 2. Summary of MR-based techniques for measuring relative temperature.

Method Principle Advantages Disadvantages References
T1 relaxation time constant As temperature increases, the motion rate increases, resulting in a greater exchange rate between water molecules. Relative temperature is measured using: ∆T = c∆T1 Readily available imaging sequences Low temperature sensitivity (1%/°C); other factors can change T1; the apparent T1 relaxation time constant is the weighted average of T1s of water molecules in tissue microstructures. This could cause a nonlinear dependence of T1 on temperature (63)
T2 relaxation time constant A linear relationship between T2 and temperature (T) exists for the free water model Can be used for adipose tissues; higher sensitivity than T1 (10%/°C) More difficult to measure than T1 due to shorter T2 values; irreversible T2w signal change at high tissue temperature due to tissue damage. (17,63,64)
Diffusion coefficient (D) The diffusion coefficient (D) is linearly related to the temperature through a Strokes-Einstein equation Readily available imaging sequences Low temperature sensitivity (2%/°C); other factors can change diffusion coefficient (D) (19,65)
Proton density (PD) Water proton density is inversely proportional to the tissue temperature Independent of tissue type; readily available imaging sequences Very low temperature sensitivity (0.29%/°C) (66)
Magnetization transfer (MT) The signal intensity, magnetization transfer ratio ((M0-MT)/M0) correlates non-linearly with tissue temperature Can be used together with other MT applications Quantitative relationship between MT signal intensity and the chemical exchange rate as a function of temperature has not been reported; non-linear function of tissue temperature; Tissue-type dependent. (67-69)
Proton resonance frequency shift (PRFS) Water hydrogen bond disruption at elevated temperature results in increased shielding constant, and thus decreased chemical shift (frequency) for water protons Fast temperature mapping techniques readily available; linear function of tissue temperature; independent of tissue type (non-fat tissue) Cannot be applied for fat tissue; relatively low temperature sensitivity (0.01 ppm/°C) (13,22,60)