有机化学英文chapter13.pptx
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1、Nuclear Magnetic ResonanceChapter 13Chapter 13第1页/共74页Molecular Spectroscopy Nuclear magnetic resonance(NMR)spectroscopyNuclear magnetic resonance(NMR)spectroscopy:a spectroscopic technique that gives us information about the number and types of atoms in a molecule,for example,about the number and t
2、ypes of hydrogen atoms using 1H-NMR spectroscopycarbon atoms using 13C-NMR spectroscopyphosphorus atoms using 31P-NMR spectroscopy第2页/共74页Nuclear Spin StatesAn electron has a spin quantum number of 1/2 with allowed values of+1/2 and-1/2 this spinning charge creates an associated magnetic fieldin eff
3、ect,an electron behaves as if it is a tiny bar magnet and has what is called a magnetic momentThe same effect holds for certain atomic nucleiany atomic nucleus that has an odd mass number,an odd atomic number,or both also has a spin and a resulting nuclear magnetic momentthe allowed nuclear spin sta
4、tes are determined by the spin quantum number,I,of the nucleus第3页/共74页Nuclear Spin Statesa nucleus with spin quantum number I I has 2 2I I +1 +1 spin states;if I =1/2,there are two allowed spin statesTable 13.1 gives the spin quantum numbers and allowed nuclear spin states for selected isotopes of e
5、lements common to organic compounds第4页/共74页Nuclear Spins in B0within a collection of 1H and 13C atoms,nuclear spins are completely random in orientationwhen placed in a strong external magnetic field of strength B0,however,interaction between nuclear spins and the applied magnetic field is quantized
6、,with the result that only certain orientations of nuclear magnetic moments are allowed 第5页/共74页Nuclear Spins in B0for 1H and 13C,only two orientations are allowed第6页/共74页Nuclear Spins in B0In an applied field strength of 7.05T,which is readily available with present-day superconducting electromagne
7、ts,the difference in energy between nuclear spin states for 1H is approximately 0.120 J(0.0286 cal)/mol,which corresponds to electromagnetic radiation of 300 MHz(300,000,000 Hz)13C is approximately 0.030 J(0.00715 cal)/mol,which corresponds to electromagnetic radiation of 75MHz(75,000,000 Hz)第7页/共74
8、页Nuclear Spin in B0the energy difference between allowed spin states increases linearly with applied field strength values shown here are for 1H nuclei第8页/共74页Nuclear Magnetic Resonancewhen nuclei with a spin quantum number of 1/2 are placed in an applied field,a small majority of nuclear spins are
9、aligned with the applied field in the lower energy statethe nucleus begins to precess and traces out a cone-shaped surface,in much the same way a spinning top or gyroscope traces out a cone-shaped surface as it precesses in the earths gravitational fieldwe express the rate of precession as a frequen
10、cy in hertz第9页/共74页Nuclear Magnetic ResonanceIf the precessing nucleus is irradiated with electromagnetic radiation of the same frequency as the rate of precession,the two frequencies couple,energy is absorbed,and the nuclear spin is flipped from spin state+1/2(with the applied field)to-1/2(against
11、the applied field)第10页/共74页Nuclear Magnetic ResonanceFigure 13.3 the origin of nuclear magnetic“resonance 第11页/共74页Nuclear Magnetic Resonance ResonanceResonance:in NMR spectroscopy,resonance is the absorption of electromagnetic radiation by a precessing nucleus and the resulting“flip”of its nuclear
12、spin from a lower energy state to a higher energy stateThe instrument used to detect this coupling of precession frequency and electromagnetic radiation records it as a signal signal:signal:a recording in an NMR spectrum of a nuclear magnetic resonance第12页/共74页Nuclear Magnetic Resonanceif we were de
13、aling with 1H nuclei isolated from all other atoms and electrons,any combination of applied field and radiation that produces a signal for one 1H would produce a signal for all 1H.The same is true of 13C nucleibut hydrogens in organic molecules are not isolated from all other atoms;they are surround
14、ed by electrons,which are caused to circulate by the presence of the applied fieldthe circulation of electrons around a nucleus in an applied field is called diamagneticdiamagnetic currentcurrent and the nuclear shielding resulting from it is called diamagnetic shieldingdiamagnetic shielding第13页/共74
15、页Nuclear Magnetic Resonancethe difference in resonance frequencies among the various hydrogen nuclei within a molecule due to shielding/deshielding is generally very smallthe difference in resonance frequencies for hydrogens in CH3Cl compared to CH3F under an applied field of 7.05T is only 360 Hz,wh
16、ich is 1.2 parts per million(ppm)compared with the irradiating frequency 第14页/共74页Nuclear Magnetic Resonancesignals are measured relative to the signal of the reference compound tetramethylsilane(TMS)for a 1H-NMR spectrum,signals are reported by their shift from the 12 H signal in TMSfor a 13C-NMR s
17、pectrum,signals are reported by their shift from the 4 C signal in TMS Chemical shift(Chemical shift():):the shift in ppm of an NMR signal from the signal of TMS第15页/共74页NMR Spectrometer第16页/共74页NMR SpectrometerEssentials of an NMR spectrometer are a powerful magnet,a radio-frequency generator,and a
18、 radio-frequency detectorThe sample is dissolved in a solvent,most commonly CDCl3 or D2O,and placed in a sample tube which is then suspended in the magnetic field and set spinningUsing a Fourier transform NMR(FT-NMR)spectrometer,a spectrum can be recorded in about 2 seconds第17页/共74页NMR Spectrum1H-NM
19、R spectrum of methyl acetate Downfield:Downfield:the shift of an NMR signal to the left on the chart paper Upfield:Upfield:the shift of an NMR signal to the right on the chart paper第18页/共74页Equivalent Hydrogens Equivalent hydrogens:Equivalent hydrogens:have the same chemical environmenta molecule wi
20、th 1 set of equivalent hydrogens gives 1 NMR signal第19页/共74页Equivalent Hydrogensa molecule with 2 or more sets of equivalent hydrogens gives a different NMR signal for each set第20页/共74页Signal AreasRelative areas of signals are proportional to the number of H giving rise to each signalModern NMR spec
21、trometers electronically integrate and record the relative area of each signal第21页/共74页ChemicalChemicalShiftsShifts1 1H-NMRH-NMR第22页/共74页Chemical Shift-1H-NMR第23页/共74页Chemical ShiftDepends on(1)electronegativity of nearby atoms,(2)the hybridization of adjacent atoms,and(3)diamagnetic effects from ad
22、jacent pi bondsElectronegativity第24页/共74页Chemical ShiftHybridization of adjacent atoms第25页/共74页Chemical ShiftDiamagnetic effects of pi bondsa carbon-carbon triple bond shields an acetylenic hydrogen and shifts its signal upfield(to the right)to a smaller valuea carbon-carbon double bond deshields vi
23、nylic hydrogens and shifts their signal downfield(to the left)to a larger value第26页/共74页Chemical Shiftmagnetic induction in the pi bonds of a carbon-carbon triple bond(Fig 13.9)第27页/共74页Chemical Shiftmagnetic induction in the pi bond of a carbon-carbon double bond(Fig 13.10)第28页/共74页Chemical Shiftma
24、gnetic induction of the pi electrons in an aromatic ring(Fig.13.11)第29页/共74页Signal Splitting;the(n+1)Rule Peak:Peak:the units into which an NMR signal is split;doublet,triplet,quartet,etc.Signal splitting:Signal splitting:splitting of an NMR signal into a set of peaks by the influence of neighboring
25、 nonequivalent hydrogens(n n+1)rule:+1)rule:if a hydrogen has n hydrogens nonequivalent to it but equivalent among themselves on the same or adjacent atom(s),its 1H-NMR signal is split into(n+1)peaks第30页/共74页Signal Splitting(n+1)1H-NMR spectrum of 1,1-dichloroethane第31页/共74页Signal Splitting(n+1)Prob
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