The absorption cross section on the ordinate of the ozone absorption spectrum is defined by Transmittance \( (T)=e^{-n \sigma b} \) where \( n \) is the number of absorbing molecules per cubic centimeter, \( \sigma \) is the absorption cross section in square centimeters \( \left(\mathrm{cm}^{2}\right) \), and \( b \) is the panthlength in centimeters \( (\mathrm{cm}) \). The total ozone in the atmosphere is approximately \( 8 \times 10^{18} \) molecules above each square centimeter of Earth's surface (from the surface up to the top of the atmosphere). If this were compressed into a pathlength of a 1-cm thick layer, the concentration would be \( 8 \times 10^{18} \) molecules \( / \mathrm{cm}^{3} \). Ultraviolet radiation in the 200 to \( 280 \mathrm{~nm} \) range is essentially completely blocked by ozone in the atmosphere but barely Harris/Lucy, Quantitative Chemical Analysis, absorbed in the 315 to \( 400 \mathrm{~nm} \) range. Based on the ozone 10e, @ 2020 W. H. Freeman and Company spectrum, the absorption cross section at 280 and \( 340 \mathrm{~nm} \) is approximately \( 40 \times 10^{-19} \mathrm{~cm}^{2} \) and \( 0.02 \times 10^{-19} \mathrm{~cm}^{2} \), Spectra of trace gases in the atmosphere. At ozone's maximum respectively. Estimate the transmittance \( (T) \) and absorbance \( (A) \quad \) opaque than a layer of gold of the same mass. [Data from U. Platt of the \( 1-\mathrm{cm}^{3} \) sample of ozone at 280 and at \( 340 \mathrm{~nm} \). and J. Stutz, Differential Absorption Spectroscopy (Berlin Heidelberg: Springer-Verlag, 2008).] \( T \) at \( 280 \mathrm{~nm}: \) Incorrect \( A \) at \( 280 \mathrm{~nm}: \) Incorrect \( T \) at \( 340 \mathrm{~nm}: \)
Sunburns are caused by the radiation in the 295-to 310 -nm region. At the center of this region, the transmittance of atmospheric ozone is \( 0.14 \). Calculate the absorption cross section for \( T=0.14, n=8 \times 10^{18} \) molecules \( / \mathrm{cm}^{3} \), and \( b=1 \mathrm{~cm} \). \( \sigma \) Incorrect By what percentage does the transmittance increase when the concentration decreases by \( 1 \% \) to \( 7.92 \times 10^{18} \) molecules/cm \( { }^{3} \) ? percentage increase: Incorrect Atmospheric \( \mathrm{O}_{3} \) is measured in Dobson units ( 1 unit \( =2.69 \times 10^{16} \) molecules \( \mathrm{O}_{3} \) above each squared centimeter of Earth's surface). (Dobson \( \equiv \) thickness [in hundredths of a millimeter] that the \( \mathrm{O}_{3} \) column would occupy if it were compressed to \( 1 \mathrm{~atm} \) at \( 0^{\circ} \mathrm{C} \).) The graph shows variations in ozone concentration as a function of latitude and season. Using an absorption cross section of \( 2.5 \times 10^{-19} \mathrm{~cm}^{2} \), calculate the transmittance in the Harris/Lucy, Quantitative Chemical Analysis, 10e, @ \( 2020 \mathrm{~W} \). H. Freeman and winter and the summer at \( 30^{\circ}-50^{\circ} \mathrm{N} \) latitude, at which \( \mathrm{O}_{3} \) varies from 290 to 350 Dobson units. Variation in atmospheric ozone at different latitudes [Data from P. S. Zurer, Chem. Eng. News, 24 May 1993 , p. 8.]
By what percentage is the ultraviolet transmittance greater in winter than in summer?