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Method Article

Near-Infrared Temperature Measurement Technique for Water Surrounding an Induction-heated Small Magnetic Sphere

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DOI:

10.3791/57407

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April 30th, 2018

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In This Article

Erratum Notice

Important: There has been an erratum issued for this article. View Erratum Notice

Summary

A technique utilizing wavelengths of 1150 and 1412 nm to measure the temperature of water surrounding an induction-heated small magnetic sphere is presented.

Abstract

A technique to measure the temperature of water and non-turbid aqueous media surrounding an induction-heated small magnetic sphere is presented. This technique utilizes wavelengths of 1150 and 1412 nm, at which the absorption coefficient of water is dependent on temperature. Water or a non-turbid aqueous gel containing a 2.0-mm- or 0.5-mm-diameter magnetic sphere is irradiated with 1150 nm or 1412 nm incident light, as selected using a narrow bandpass filter; additionally, two-dimensional absorbance images, which are the transverse projections of the absorption coefficient, are acquired via a near-infrared camera. When the three-dimensional distributions of temperature can be assumed to be spherically symmetric, they are estimated by applying inverse Abel transforms to the absorbance profiles. The temperatures were observed to consistently change according to time and the induction heating power.

Introduction

A technique to measure temperature near a small heat source within a medium is required in many scientific research fields and applications. For example, in the research on magnetic hyperthermia, which is a cancer therapy method using electromagnetic induction of magnetic particles, or small magnetic pieces, it is critical to accurately predict the temperature distributions generated by the magnetic particles1,2. However, although microwave3,4, ultrasound5,6,7....

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Protocol

1. Experimental Setup and Procedures

Prepare an optical rail to mount a sample and optics for NIR imaging as follows.

  1. Sample preparation.
    Note: When using water or aqueous liquid, do Step 1.1.1. When using an aqueous gel with high viscosity, do Step 1.1.2.
    1. Steel sphere setting in water.
      1. Fix a 2.0-mm-diameter steel sphere to the end of a thin plastic string using a small amount of glue.
      2. Hang the steel sphere at the center of the rectangular glass cell with an optical path length of 10.0 mm, a width of 10 mm, and a height of 45 mm (Figure 3).....

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Results

Images of ΔAi(x, z) at λ = 1150 nm for a 2.0-mm-diameter steel sphere in water and at λ = 1412 nm for a 0.5-mm-diameter steel sphere in maltose syrup are presented in Figure 5a and Figure 6a, respectively. In both cases, the sphere was located 12 mm below the bottom of the coil along its central axis. Figure 5

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Discussion

The technique presented in this paper is a novel one using the temperature dependence of NIR absorption of water and presents no significant difficulty in setting up the necessary equipment and implementation. The incident light can be easily produced by using a halogen lamp and an NBPF. However, lasers cannot be used, because coherent interference patterns would appear on the images. Common optical lenses and glass cells for visible-light use can be used, as they transmit an adequate amount of light at λ =.......

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Disclosures

The authors have nothing to disclose.

Acknowledgements

The authors thank Mr. Kenta Yamada, Mr. Ryota Fujioka, and Mr. Mizuki Kyoda for their support on the experiments and data analyses. This work was supported by JSPS KAKENHI Grant Number 25630069, the Suzuki Foundation, and the Precise Measurement Technology Promotion Foundation, Japan.

....

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Materials

List of materials used in this article
NameCompanyCatalog NumberComments
Induction heating systemCEIA, ItalySPW900/56780 kHz, 5.6 kW (max).
CoilSA-JapancustomWater-cooled copper tube; two-turn; outer dia. 28 mm.
Water chillerMatsumoto Kikai, JapanMP-401CT
Halogen lampHayashi Watch-Works, JapanLA-150UE-A
Narrow bandpass filter for λ = 1150 nmAndover115FS10-25Full width at half-maximum (FWHM): 10 nm.
Narrow bandpass filter for λ = 1412 nmAndoversemi-customFull width at half-maximum (FWHM): 10 nm.
Bandpass filter for λ = 850−1300 nmSpectrogonSP-1300
Bandpass filter for λ = 1100−2000 nmSpectrogonSP-2000
NIR cameraFLIR SystemsAlpha NIRInGaAs
Image acquisition softwareFLIR SystemsIRvista
Image processing softwareNIHImageJver. 1.51r
Image processing softwareMathWorksMatlabver. 2016a
Telecentric lensEdmond Optics55350-LX1
Steel sphere (0.5 mm dia.)Kobe Steel, JapanFe-1.5Cr-1.0C-0.4Mn (wt %)
Steel sphere (2.0 mm dia.)Kobe Steel, JapanFe-1.5Cr-1.0C-0.4Mn (wt %)
Maltose syrup as aqueous gelSonton, JapanMizuameFood product

References

  1. Physics of Thermal Therapy. Moros, E. G. , CRC Press. (2012).
  2. Périgo, E. G., Hemery, G., Sandre, O., Ortega, D., Garaio, E., Plazaola, F., Teran, F. J. Fundamentals and advances in magnetic hyperthermia. Appl Phys Rev. 2, 041302(2015).
  3. Bardati, F., Marrocco, G., Tognolatti, P. Time-dependent microwave radiometry for the measurement of temperature in medic....

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Erratum


Formal Correction: Erratum: Near-Infrared Temperature Measurement Technique for Water Surrounding an Induction-heated Small Magnetic Sphere
Posted by JoVE Editors on 12/06/2018. Citeable Link.

An erratum was issued for: Near-Infrared Temperature Measurement Technique for Water Surrounding an Induction-heated Small Magnetic Sphere. The Protocol section was updated.

In 2.2.7, the temperature coefficient of water, αf, for λ = 1150 nm has been corrected from:

4.0 x 10-3 K-1 mm-1

to:

2.8 x 10-4 K-1 mm-1

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