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Series Pfund

Figure 1.1 Energy levels (vertical lines) and observed transitions (horizontal lines) of the hydrogen atom, including the Lyman, Balmer, Paschen, Brackett and Pfund series... Figure 1.1 Energy levels (vertical lines) and observed transitions (horizontal lines) of the hydrogen atom, including the Lyman, Balmer, Paschen, Brackett and Pfund series...
Eventually, other series of lines were found in other regions of the electromagnetic spectrum. The Lyman series was observed in the ultraviolet region, whereas the Paschen, Brackett, and Pfund series were observed in the infrared region of the spectrum. All of these lines were observed as they were emitted from excited atoms, so together they constitute the emission spectrum or line spectrum of hydrogen atoms. [Pg.9]

The Lyman, Balmer, Paschen, Brackett and Pfund series... [Pg.58]

There are in principle an infinite number of series beginning at higher quantum numbers with i = 6, 7, 8, 9... but they become increasingly difficult to observe. For the higher n series to be seen in the spectrum the levels have to be populated, so some hydrogen atoms must be in the n = 5 level to see the Pfund series. We shall see that the presence of the Balmer series in the spectrum of a star is indicative of the stellar temperature, which is a direct consequence of the population of the energy levels. More of this in Chapter 4. [Pg.59]

Pfund series The series of the hydrogen atom spectrum with n = 5 as the starting level. [Pg.314]

Pfund series spect A series of lines in the infrared spectrum of atomic hydrogen whose wave numbers are given by Rh (1/25) - (l/n ), where Rh is the Rydberg constant for hydrogen, and n is any integer greater than 5. fiint, sir-ez ... [Pg.284]

Lyman series, far ultraviolet. Paschen series, far infrared, Brackett series, far infrared, Pfund series, far infrared. [Pg.160]

Subsequent to the discovery of the Balmer series of lines in the visible region of the electromagnetic spectrum, it was found that many other spectral lines are also present in nonvisible regions of the electromagnetic spectrum. Hydrogen, for example, shows a series of spectral lines called the Lyman series in the ultraviolet region and still other series (the Paschen, Brackett, and Pfund series) in the infrared region. [Pg.165]

What is the shortest wavelength (in nanometers) in the Pfund series (Problem 5.89) for hydrogen ... [Pg.196]

Eventually, this series of lines became known as the Balmer series. Balmer wondered whether his little formula might be extended to study the spectra of other elements. He knew similar patterns exist in the line spectra of many elements. He also wondered about spectral lines that the human eye can t see. A few years later, in 1906, additional series of lines were in fact discovered for hydrogen in the ultraviolet region of the spectrum. These were called the Lyman series after their discoverer, Theodore Lyman. Other famous series are the Paschen series, named after German scientist Friedrich Paschen, the Brackett series, named after U.S. scientist F. S. Brackett, and the wonderful Pfund series, named after U.S. scientist August Herman Pfund. The Paschen, Brackett, and Pfund series lie in the infrared region. ... [Pg.26]

Figure 2.10 Energy-level diagram for hydrogen showing several transitions in the Lyman, Balmer, Paschen, and Brackett series. The Pfund series, not shown, corresponds to transitions to the fifth energy level. Figure 2.10 Energy-level diagram for hydrogen showing several transitions in the Lyman, Balmer, Paschen, and Brackett series. The Pfund series, not shown, corresponds to transitions to the fifth energy level.
Pfund Series This series formed when excited electrons in hydrogen atom fall from higher energy levels to fifth energy level. It lies in infrared region. [Pg.260]

Comparison with the empirical Equation (1.4) shows that RH = fie4/8h3 and that n" = 2 for the Balmer series. Similarly n" = 1, 3, 4, and 5 for the Lyman, Paschen, Brackett and Pfund series, although it is important to realize that there is an infinite number of series. Many series with high n" have been observed, by techniques of radioastronomy, in the interstellar medium, where there is a large amount of atomic hydrogen. For example, the (n = 167) — (n" = 166) transition5 has been observed with v= 1.425 GHz (2 = 21.04 cm). [Pg.5]

Each set of arrows in step 2 represents a spectral emission series. Label five of the series, from greatest energy change to least energy change, as the Lyman, Balmer, Paschen, Brackett, and Pfund series. [Pg.130]

Aware of only these four hues, Balmer calculated 1 for a fifth hue lyn = 7). A hue with a wavelength very close to the predicted value was observed experimentally. Balmer suggested that his formula might also predict wavelengths of other series of spectral fines by using integer values for n other than 2 and rw n L 1. Other series of hydrogen lines were not known then, but were subsequently discovered (the Lyman, Paschen, Brackett, and Pfund series of fines). [Pg.131]

Other series of spectral lines occur in the ultraviolet (Lyman series) and infrared (Paschen, Brackett and Pfund series). All lines in all the series obey the general expression given in equation 1.5 where n > n. For the Lyman series, n=, for the Balmer series, n = 2, and for the Paschen, Brackett and Pfund series, k = 3, 4 and 5 respectively. Figure 1.3 shows some of the allowed transitions of the Lyman and Balmer series in the emission spectrum of atomic H. Note the use of the word allowed, the transitions must obey selection... [Pg.5]

Equation (2-6) led to the identification of other series of the lines for hydrogen, including the Paschen series (n = 3), the Brackett series (nj = 4), and the Pfund series (n = 5). The Balmer series is in the visible region of the spectrum, the Lyman series is in the ultraviolet, and the Paschen, Brackett, and Pfund series appear in the infrared. Their distribution is shown in Figure 2-2. Equation (2-6), which accounts for all presently known lines of hydrogen, led Ritz (1908) to propose his combination principle, that the wavenumbers of all lines in a series are the result of the difference in energy between a fixed and a running term. [Pg.17]

Representative emission spectra are shown schematically in Fig. 2.2 for hydrogen, potassium, and mercury on a common wavelength scale from the near infrared to the ultraviolet. Under the coarse wavelength resolution of this figure, the emitted light intensities are concentrated at single, well-defined emission lines. In H, the displayed emission consists of four convergent series of lines, the so-called Ritz-Paschen and Pfund series in the near infrared, the Lyman series in the vacuum ultraviolet, and the Balmer series in the visible. Johann Balmer, a schoolteacher in Basel in the late nineteenth century. [Pg.34]


See other pages where Series Pfund is mentioned: [Pg.50]    [Pg.159]    [Pg.188]    [Pg.59]    [Pg.283]    [Pg.196]    [Pg.27]    [Pg.188]    [Pg.4]    [Pg.188]    [Pg.5]    [Pg.103]    [Pg.517]    [Pg.257]    [Pg.138]    [Pg.406]    [Pg.615]    [Pg.110]    [Pg.4]   
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