Sakuma–Hattori equation explained

In physics, the Sakuma–Hattori equation is a mathematical model for predicting the amount of thermal radiation, radiometric flux or radiometric power emitted from a perfect blackbody or received by a thermal radiation detector.

History

The Sakuma–Hattori equation was first proposed by Fumihiro Sakuma, Akira Ono and Susumu Hattori in 1982. In 1996, a study investigated the usefulness of various forms of the Sakuma–Hattori equation. This study showed the Planckian form to provide the best fit for most applications. This study was done for 10 different forms of the Sakuma–Hattori equation containing not more than three fitting variables. In 2008, BIPM CCT-WG5 recommended its use for radiation thermometry measurement uncertainty budgets below 960 °C.

General form

The Sakuma–Hattori equation gives the electromagnetic signal from thermal radiation based on an object's temperature. The signal can be electromagnetic flux or signal produced by a detector measuring this radiation. It has been suggested that below the silver point, a method using the Sakuma–Hattori equation be used.^[1] In its general form it looks like^[2] $$S(T)\; =\; \backslash frac,$$where:

C is the scalar coefficientc _{2} is the second radiation constant (0.014387752 m⋅K^[3])λ _{x} is the temperature-dependent effective wavelength (in meters)T is the absolute temperature (in K)

Planckian form

Derivation

The Planckian form is realized by the following substitution:$$\backslash lambda\; \_x\; =\; A\; +\; \backslash frac$$

Making this substitution renders the following the Sakuma–Hattori equation in the Planckian form.

Sakuma–Hattori equation (Planckian form)

S(T) = (C)/(\exp\left( (c _{2})/(\right) -1 AT + B))

Inverse equation

T = (c _{2})/(A ln \left( (C)/(S) + 1 \right)) - (B)/(A)

First derivative^[4]

(dS)/(dT) = \left[S(T)\right] ^{2} (A c _{2})/(\exp\left( C\left(AT + B\right) ^{2}) (c _{2})/(AT + B) \right)

Discussion

The Planckian form is recommended for use in calculating uncertainty budgets for radiation thermometry^[2] and infrared thermometry.^[5] It is also recommended for use in calibration of radiation thermometers below the silver point.^[2]

The Planckian form resembles Planck's law.

$$S(T)\; =\; \backslash frac$$

However the Sakuma–Hattori equation becomes very useful when considering low-temperature, wide-band radiation thermometry. To use Planck's law over a wide spectral band, an integral like the following would have to be considered:

$$S(T)\; =\; \backslash int\_^\backslash frac\; d\backslash lambda$$

This integral yields an incomplete polylogarithm function, which can make its use very cumbersome.The standard numerical treatment expands the incomplete integral in a geometric series of the exponential$$\backslash int\_0^\; \backslash frac\; d\backslash lambda=\; c\_1\; \backslash left(\backslash frac\backslash right)^4\backslash int\_^\backslash infty\; \backslash frac\; dx$$after substituting

λ = \tfrac{c _{2}{xT},} d λ = \tfrac{ - c ^{2} _{2 }{x} T dx}. Thenprovides an approximation if the sum is truncated at some order.

The Sakuma–Hattori equation shown above was found to provide the best curve-fit for interpolation of scales for radiation thermometers among a number of alternatives investigated.^[6]

The inverse Sakuma–Hattori function can be used without iterative calculation. This is an additional advantage over integration of Planck's law.

Other forms

The 1996 paper investigated 10 different forms. They are listed in the chart below in order of quality of curve-fit to actual radiometric data.^[6]

Name	Equation	Bandwidth	Planckian
Sakuma–Hattori Planck III	S(T) = (C)/(\exp\left( (c _{2})/(\right) -1 AT + B))	narrow	yes
Sakuma–Hattori Planck IV	S(T) = (C)/(\exp\left( (A)/(+ (B)/(2 T) \right) -1 T ^{2}))	narrow	yes
Sakuma–Hattori – Wien's II	S(T) = C \exp\left( (- c _{2})/(AT + B) \right)	narrow	no
Sakuma–Hattori Planck II	S(T) = (C T ^{A})/(\exp\left( (B)/(\right) -1 T))	broad and narrow	yes
Sakuma–Hattori – Wien's I	S(T) = C T ^{A} {\exp\left( (- B)/(T) \right)}	broad and narrow	no
Sakuma–Hattori Planck I	S(T) = (C)/(\exp\left( (c _{2})/(\right) -1 AT))	monochromatic	yes
New	S(T) = C \left( 1 + (A)/(T) \right) - B	narrow	no
Wien's	S(T) = C \exp\left( (- c _{2})/(A T) \right)	monochromatic	no
Effective Wavelength – Wien's	S(T) = C \exp\left( (- A)/(+ T) (B)/(T ^{2}) \right)	narrow	no
Exponent	S(T) = C T ^{A}	broad	no

See also

• Stefan–Boltzmann law
• Planck's law
• Rayleigh–Jeans law
• Wien approximation
• Wien's displacement law
• Kirchhoff's law of thermal radiation
• Infrared thermometer
• Pyrometer
• Thin-filament pyrometry
• Thermography
• Black body
• Thermal radiation
• Radiance
• Emissivity
• ASTM Subcommittee E20.02 on Radiation Thermometry

References

1. Book: F. . Sakuma . S. . Hattori . Establishing a practical temperature standard by using a narrow-band radiation thermometer with a silicon detector . Temperature: Its Measurement and Control in Science and Industry . 5 . J. F. . Schooley . New York . AIP . 421–427 . 1982 . 0-88318-403-6 .
2. J. . Fischer . P. . Saunders . M. . Sadli . M. . Battuello . C. W. . Park . Y. . Zundong . H. . Yoon . W. . Li . E. . van der Ham . F. . Sakuma . Y. . Yamada . M. . Ballico . G. . Machin . N. . Fox . J. . Hollandt . M. . Matveyev . P. . Bloembergen . S. . Ugur . Uncertainty budgets for calibration of radiation thermometers below the silver point . CCT-WG5 on Radiation Thermometry, BIPM, Sèvres, France . 2008 . 29 . 3 . 1066 . 10.1007/s10765-008-0385-1 . 2008IJT....29.1066S . 122082731 . 1 .
3. Web site: National Institute of Standards and Technology (NIST) . 2006 CODATA recommended values . Dec 2003 . Apr 27, 2010.
4. ASTM Standard E2758-10 – Standard Guide for Selection and Use of Wideband, Low Temperature Infrared Thermometers, ASTM International, West Conshohocken, PA, (2010).

   Updated: ASTM E2758-15a(2021), https://www.astm.org/e2758-15ar21.html

5. MSL Technical Guide 22 – Calibration of Low Temperature Infrared Thermometers (pdf), Measurement Standards Laboratory of New Zealand (2008). Updated: Version 3. July 2019, https://www.measurement.govt.nz/download/28
6. Sakuma F, Kobayashi M., "Interpolation equations of scales of radiation thermometers", Proceedings of TEMPMEKO 1996, pp. 305–310 (1996).