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Page: 354 More than a thousand different chemical compounds have been isolated from coffee. Their structures were determined using various spectroscopic techniques.
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Page: 356 FIGURE 12-1 A representation of an electron-ionization, magnetic-sector mass spectro meter. Molecules are ionized by collision with high-energy electrons, causing some of the molecules to fragment. Passage of the charged fragments through a magnetic field then sorts them according to their mass.
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Page: 356 FIGURE 12-2 A representation of a quadrupole mass analyzer. Only ions of a certain m/z ratio will reach the detector; other ions with unstable trajectories will collide with the rods.
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Page: 357 FIGURE 12-3 Mass spectrum of propane (C3H8; MW 5 44).
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Page: 358 FIGURE 12-4 Mass spectrum of 2,2-dimethylpropane (C5H12; MW 5 72). No molecular ion is observed when electron-impact ionization is used. What do you think is the formula and structure of the M1 peak at m/z 5 57?
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Page: 359 FIGURE 12-5 Mass spectrum of hexane (C6H14; MW 5 86). The base peak is at m/z 5 57, and numerous other ions are present.
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Page: 360 FIGURE 12-6 Fragmentation of hexane in a mass spectrometer.
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Page: 360 FIGURE 12-7 Mass spectra of unlabeled samples A and B for Worked Example 12-1.
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Page: 361 FIGURE 12-8 Mass spectra for Problem 12-2.
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Page: 362 FIGURE 12-9 Mass spectrum of 2-pentanol.
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Page: 363 FIGURE Mass spectrum of triethylamine.
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Page: 364 FIGURE Mass spectrum of chloroethane.
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Page: 364 FIGURE Mass spectrum of 1-bromohexane.
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Page: 365 FIGURE Mass spectrum of butyrophenone.
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Page: 366 FIGURE Mass spectrum of 2-methyl-3-pentanol, Worked Example 12-2.
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Page: 368 FIGURE MALDI–TOF mass spectrum of chicken egg-white lysozyme. The peak at 14, daltons (amu) is due to the monoprotonated protein, M+H+, and the peak at 28, daltons is due to an impurity formed by dimerization of the protein. Other peaks at lower m/z values are various protonated species, M+Hnn+.
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Page: 368 FIGURE The electro-magnetic spectrum covers a continuous range of wavelengths and frequencies, from radio waves at the low-frequency end to gamma (y) rays at the high-frequency end. The familiar visible region accounts for only a small portion near the middle of the spectrum.
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Page: 369 FIGURE Electromagnetic waves are characterized by a wavelength, a frequency, and an amplitude. (a) Wavelength (λ) is the distance between two successive wave maxima. Amplitude is the height of the wave measured from the center. (b)–(c) What we perceive as different kinds of electromagnetic radiation are simply waves with different wavelengths and frequencies.
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Page: 370 FIGURE An infrared absorption spectrum for ethanol, CH3CH2OH. A transmittance of 100% means that all the energy is passing through the sample, whereas a lower transmittance means that some energy is being absorbed. Thus, each downward spike corresponds to an energy absorption.
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Page: 372 FIGURE The infrared and adjacent regions of the electromagnetic spectrum.
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Page: 374 FIGURE IR spectra of (a) hexane, (b) 1-hexene, and (c) 1-hexyne. Spectra like these are easily obtained from submilligram amounts of material in a few minutes using commercially available instruments.
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Page: 375 FIGURE The four regions of the infrared spectrum: single bonds to hydrogen, triple bonds, double bonds, and fingerprint.
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Page: 378 FIGURE C – H out-of-plane bending vibrations for substituted alkenes.
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Page: 379 FIGURE C – H out-of-plane bending vibrations for substituted benzenes.
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Page: 380 FIGURE IR spectrum of cyclohexanol.
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Page: 380 FIGURE IR spectrum of cyclohexylamine.
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Page: 381 FIGURE The IR spectrum of benzaldehyde.
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Page: 382 FIGURE IR spectrum for Worked Example 12-6.
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Page: 383 FIGURE The IR spectrum of phenylacetylene, Problem 12-9.
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Page: 384 The structure of human muscle fructose-1,6-bisphosphate aldolase, as determined by X-ray crystallography and downloaded from the Protein Data Bank, 1ALD.
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