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Possible temperature effects computed for acoustic microscopy used for living cells
T Kujawska1, J Wójcik, L Filipczyński
1Institute of Fundamental Technological Research, Polish Academy of Sciences, Warsaw, Poland.
Ultrasound in Medicine & Biology
|February 14, 2004
Summary
High-frequency ultrasound microscopy (GHz) can damage living cells due to temperature increases. This study models temperature distributions, finding that water absorption significantly impacts heating, and lower frequencies and powers reduce thermal effects for safer cell imaging.
Area of Science:
- Biophysics
- Acoustic Microscopy
- Cellular Imaging
Background:
- High-frequency ultrasound microscopy (GHz) enables advanced biological applications.
- Potential temperature increases from focused ultrasonic beams pose a risk to living cells.
- Limited data exists on local temperature rises due to nonlinear propagation effects at GHz frequencies.
Purpose of the Study:
- To numerically compute temperature distributions in a water medium simulating living cells at 1 GHz.
- To investigate the influence of nonlinear propagation effects and transducer power on temperature increases.
- To assess the impact of water absorption and repetition frequency on thermal effects.
Main Methods:
- Numerical solution of temperature distributions at 1 GHz using water as a model for acoustic parameters.
- Simulation of high (0.32 W) and low (0.002 W) transducer powers.
- Calculation of pressure distributions and effective focal radius for fundamental and harmonic frequencies.
Main Results:
- Focal temperature increase reached 14°C at 10 MHz repetition frequency and 0.32 W transducer power.
- Maximum temperature increase of 20°C occurred at the sapphire lens-water boundary.
- Water's high absorption significantly suppressed focal temperature peaks; temperature increases are proportional to repetition frequency.
Conclusions:
- At practical repetition frequencies (e.g., 0.1 MHz), temperature increases are substantially lower.
- Lower transducer power (0.002 W) resulted in approximately 140 times lower temperature increases compared to high power.
- Effective focal radius was 1.1 µm at 1 GHz and 0.7 µm for the second harmonic, independent of transducer power.