Optical detection of the ultrasound-induced pulsed thermal lens close to the ice-water phase transition

G. A. S. Flizikowski; E. V. Bergmann; A. Bazachi; R. S. Mendes; A. Novatski; C. Jacinto; M. L. Baesso; L. C. Malacarne; N. G. C. Astrath

doi:10.1364/AO.496255

Applied Optics
Vol. 62,
Issue 19,
pp. 5094-5098
(2023)
•https://doi.org/10.1364/AO.496255

Optical detection of the ultrasound-induced pulsed thermal lens close to the ice-water phase transition

G. A. S. Flizikowski, E. V. Bergmann, A. Bazachi, R. S. Mendes, A. Novatski, C. Jacinto, M. L. Baesso, L. C. Malacarne, and N. G. C. Astrath

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
G. A. S. Flizikowski, E. V. Bergmann, A. Bazachi, R. S. Mendes, A. Novatski, C. Jacinto, M. L. Baesso, L. C. Malacarne, and N. G. C. Astrath, "Optical detection of the ultrasound-induced pulsed thermal lens close to the ice-water phase transition," Appl. Opt. 62, 5094-5098 (2023)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Check for updates

Abstract

Piezo-optic and thermo-optic coefficients are important material properties that play a critical role in the design and optimization of many optical devices. The ability to accurately measure and control these coefficients is essential for achieving high performance and reliability in a wide range of applications. In this article, we use the optical detection of the ultrasound-induced thermal lens effect to investigate these properties for water at low temperatures. The results show that the anomalous behavior of water around 4°C is easily observed. The thermal lens method is used to determine the temperature dependence of the piezo-optic and thermo-optic coefficients.

Full Article | PDF Article

More Like This

Induction and detection of pressure waves by pulsed thermal lens technique in water–ethanol mixtures

Otávio A. Capeloto, Vitor S. Zanuto, Vinicius G. Camargo, Gabriel A. S. Flizikowski, Flávia A. P. Morais, Gustavo V. B. Lukasievicz, Leandro S. Herculano, Marcos P. Belançon, Nelson G. C. Astrath, and Luis C. Malacarne
Appl. Opt. 60(13) 4029-4033 (2021)

Nanosecond pressure transient detection of laser-induced thermal lens

Otávio A. Capeloto, Vitor S. Zanuto, Vinicius G. Camargo, Gabriel A. S. Flizikowski, Gustavo V. B. Lukasievicz, Leandro S. Herculano, Marcos P. Belançon, Nelson G. C. Astrath, and Luis C. Malacarne
Appl. Opt. 59(12) 3682-3685 (2020)

Pulsed mode thermal lens effect detection in the near field via thermally induced probe beam spatial phase modulation: a theory

J. F. Power
Appl. Opt. 29(1) 52-63 (1990)

Previous Article Next Article

Data availability

Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Figures (2)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (2)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Equations (8)

You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

T	$ρ$	$k_{t h}$	$c_{p}$	$β$	$c_{s}$
°C	${k g / m}^{3}$	$W / m . K$	$J / k g . K$	$10^{- 5} 1 / K$	$m / s$
0	999.84	0.556	4217.74	−6.814	1402.06
2	999.94	0.561	4210.74	−3.277	1411.75
4	999.97	0.565	4204.84	−0.003	1421.03
6	999.94	0.570	4199.87	3.122	1429.90
10	999.70	0.578	4192.21	8.790	1446.46
15	999.10	0.588	4185.81	15.073	1465.17
20	998.21	0.598	4181.87	20.661	1481.74
25	997.05	0.606	4179.61	25.705	1496.36

T	$- d n / d T$	$d n / d p$
°C	$10^{- 5} 1 / K$	$10^{- 10} 1 / P a$
0	$0.040 \pm 0.005$	$1.57 \pm 0.07$
2	$1.52 \pm 0.07$	$1.55 \pm 0.07$
4	$2.2 \pm 0.1$	$1.53 \pm 0.07$
6	$3.4 \pm 0.2$	$1.51 \pm 0.07$
10	$4.8 \pm 0.2$	$1.47 \pm 0.06$
15	$7.1 \pm 0.3$	$1.44 \pm 0.06$
20	$8.8 \pm 0.4$	$1.41 \pm 0.06$
25	$10.6 \pm 0.5$	$1.38 \pm 0.06$

T	$ρ$	$k_{t h}$	$c_{p}$	$β$	$c_{s}$
°C	${k g / m}^{3}$	$W / m . K$	$J / k g . K$	$10^{- 5} 1 / K$	$m / s$
0	999.84	0.556	4217.74	−6.814	1402.06
2	999.94	0.561	4210.74	−3.277	1411.75
4	999.97	0.565	4204.84	−0.003	1421.03
6	999.94	0.570	4199.87	3.122	1429.90
10	999.70	0.578	4192.21	8.790	1446.46
15	999.10	0.588	4185.81	15.073	1465.17
20	998.21	0.598	4181.87	20.661	1481.74
25	997.05	0.606	4179.61	25.705	1496.36

T	$- d n / d T$	$d n / d p$
°C	$10^{- 5} 1 / K$	$10^{- 10} 1 / P a$
0	$0.040 \pm 0.005$	$1.57 \pm 0.07$
2	$1.52 \pm 0.07$	$1.55 \pm 0.07$
4	$2.2 \pm 0.1$	$1.53 \pm 0.07$
6	$3.4 \pm 0.2$	$1.51 \pm 0.07$
10	$4.8 \pm 0.2$	$1.47 \pm 0.06$
15	$7.1 \pm 0.3$	$1.44 \pm 0.06$
20	$8.8 \pm 0.4$	$1.41 \pm 0.06$
25	$10.6 \pm 0.5$	$1.38 \pm 0.06$

G. A. S. Flizikowski	https://orcid.org/0000-0003-1534-6437
L. C. Malacarne	https://orcid.org/0000-0002-9436-6497
N. G. C. Astrath	https://orcid.org/0000-0002-1658-8043

Abstract

Data availability

Cited By

Figures (2)

Tables (2)

Equations (8)

Applied Optics