Wein’s law establishes a link between the wavelength of light with the greatest intensity and the object’s absolute temperature.
In other words, Wein’s displacement rule explains why things produce a spectrum of distinct wavelengths at different temperatures. For example, hotter items emit shorter wavelengths, which gives them a reddish hue, but cooler objects emit longer wavelengths, which gives them a blue hue.
Wien’s law
When the temperature of a blackbody radiator rises, the total amount of energy emitted increases and the radiation curve’s peak shifts to shorter wavelengths. When the maximum is calculated using the Planck radiation formula, it is discovered that the product of the peak wavelength and temperature is constant.
Mathematical representation of the law:
λₘT = b
Where,
- λₘ is the maximum wavelength that corresponds to the greatest intensity
- b is the Wien’s displacement constant = 2.8977*103 m.K
- T is the temperature in kelvins
Wien’s constant is a physical constant that defines the connection between the thermodynamic temperature of a black body and its wavelength. It is a product of temperature and the black body’s wavelength, which decreases as the wavelength approaches its maximum value with temperature.
The Derivation of Wien’s Displacement Law
William Wiens utilised thermodynamics to explain the distribution of wavelengths in relation to the energy released by radiations, coining the term Wien’s law of distribution. According to Wien’s distribution, the energy distribution varies in proportion to λ-5.
For small values of λ, the exponential component becomes significant and contributes more than the other factor λ-5. This suggests that E grows as λ decreases at shorter wavelengths. On the other hand, when λ increases, the exponential factor becomes extremely tiny. In this range, dominating is the case, and hence E should be reduced as λ increases.
At first glance, Wien’s law appears to be an adequate explanation for the blackbody radiation curve. However, compare the curve displayed by Wien’s distribution law to the experimental curve. As we can see, Wien’s law fits extremely well in the lower A range, but there is a discrepancy between both curves in the higher A range. This implies an error in the theoretical distribution law that is too great to be accounted for by experimental uncertainty, indicating a theoretical problem. Wien was unable to explain his relationship’s collapse or provide a replacement.
Although Wien’s law does not provide a comprehensive explanation, the following may be used to determine the maximum spectral emissive power dependency on temperature:
We have at λ = λₘ, λₘT = b, from Wien’s displacement law
Where,
- λₘ – The wavelength that corresponds to the highest intensity.
- T – The absolute temperature
b – Wein’s Constant and its value are provided by 2.88 x 10-³ m-K or 0.288 cm-K
Limitations of Wien’s displacement law
The constraint on Wien’s displacement law implies that it fails in the presence of longer wavelength blackbody radiations. When the body’s temperature is lowered, a continuous Wein curve is impossible to obtain.
The Importance of Wien’s Displacement
We may use Wien’s displacement law to calculate the temperature of celestial objects. It is employed in the development of remote sensors. Additional uses of Wien’s displacement rule include the following:
- Incandescent Bulb Light: As the filament’s temperature decreases, the wavelengths of light get longer, making the light look redder.
- The Sun’s Temperature: Using a wavelength of 500 nm in the green spectrum, which is visible to the human eye, one may investigate the sun’s peak emission per nanometre.
Conclusion
At the dawn of quantum mechanics, the primary difficulty for physicists was to explain the wave character of atoms. In quantum physics, black body radiation is critical. At absolute zero temperature, black substances absorb all radiations, i.e., there is no transmission or emission of radiations. Numerous scientists have contributed to the understanding of black body radiations.
Max Planck quantified black body radiation, whereas Rayleigh-Jeans and Wein’s provided exceptions to Planck’s law. For shorter wavelengths, Wein’s law was developed, whereas Rayleigh-Jeans described it for longer wavelengths. However, Wein’s law predates Max Planck’s explanation.