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Return to NMR Spectroscopy in Inorganic Chemistry 2e Student resources
Chapter 7 Multiple Choice Questions
The solid state
Quiz Content
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not completed
.
The nuclear spin Hamiltonian includes components Ĥ
ext
and Ĥ
int
, where
Ĥ
ext
describes the interaction with the spectrometer magnetic field B
0
, while Ĥ
int
describes the interactions between spins.
correct
incorrect
Ĥ
ext
describes the interaction of the spins with the pulses B
1
used to excite the nuclear spins. Ĥ
int
describes the interaction of the spins with the spectrometer magnetic field B
0
.
correct
incorrect
Ĥ
ext
describes the interaction of the spins with the spectrometer magnetic field B
0
and with the pulses B
1
used to excite the nuclear spins. Ĥ
int
describes the interaction between spins.
correct
incorrect
Ĥ
ext
describes the interaction of the spins with the spectrometer magnetic field B
1
, while Ĥ
int
describes the interaction with the pulses B
1
used to excite the nuclear spins.
correct
incorrect
*
not completed
.
Anisotropic components of Ĥ
int
, i.e., those that depend on the orientation of the individual molecule with respect to the spectrometer magnetic field B
0
, are due to
chemical shift, dipolar and quadrupolar interactions.
correct
incorrect
chemical shift, scalar coupling and spin rotation.
correct
incorrect
spin rotation, scalar coupling and quadrupolar interactions.
correct
incorrect
chemical shift and scalar coupling.
correct
incorrect
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not completed
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Solid-state NMR spectra measured without magic angle spinning
give results identical to those measured with magic angle spinning.
correct
incorrect
can be measured but the resulting spectra will differ from those measured with magic angle spinning.
correct
incorrect
can only be obtained for spin ½ nuclei, and the results will differ from those measured with magic angle spinning.
correct
incorrect
cannot be measured.
correct
incorrect
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not completed
.
Magic angle spinning
averages to zero the contribution of chemical shift anisotropy, reduces both dipolar and some quadrupolar interactions, making the resonances in solid-state spectra sharper.
correct
incorrect
averages to zero the contribution of chemical shift anisotropy, making resonances in solid-state spectra broader.
correct
incorrect
averages to zero the contribution of chemical shift anisotropy and reduces both dipolar and quadrupolar interactions, making resonances in solid-state spectra broader.
correct
incorrect
does not impact on the overall appearance of the solid-state spectra.
correct
incorrect
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not completed
.
Spinning the sample more slowly than the width of the static lineshape of the signal in Hz
results in a sharper resonance at the isotropic chemical shift due to removal of spinning sidebands.
correct
incorrect
results in a broader resonance at the isotropic chemical shift accompanied by spinning sidebands.
correct
incorrect
results in a sharper resonance at the anisotropic chemical shift and the presence of the spinning sidebands.
correct
incorrect
does not have any effect on the linewidth of the resonance.
correct
incorrect
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not completed
.
One of the ways to remove dipolar interactions from solid-state
1
H NMR spectra is to
combine fast magic angle spinning, isotopic dilution and use a very high magnetic field spectrometer.
correct
incorrect
use fast magic angle spinning and a very low magnetic field spectrometer.
correct
incorrect
combine isotropic dilution with a very high magnetic field spectrometer and record spectra without magic angle spinning.
correct
incorrect
combine slow magic angle spinning, isotopic dilution and use a very low magnetic field spectrometer.
correct
incorrect
*
not completed
.
Hartmann-Hahn matching is the basis of cross-polarisation and allows
polarisation transfer via the quadrupolar interaction between more sensitive spins
I
and a less sensitive spin
S
aimed to improve the sensitivity of measurements of spin
S
.
correct
incorrect
polarisation transfer via the dipolar coupling between a more sensitive spin
S
and a less sensitive spin
I
to improve the sensitivity in measurements of spin
S
.
correct
incorrect
polarisation transfer via the dipolar coupling between a more sensitive spin
I
and a less sensitive spin
S
to improve the sensitivity in measurements of spin
I
.
correct
incorrect
polarisation transfer via the dipolar coupling between a more sensitive spin
I
and a less sensitive spin
S
to improve the sensitivity in measurements of spin
S
.
correct
incorrect
*
not completed
.
The most commonly used spin
I
in cross-polarisation experiments is
1
H due to its high natural abundance and large gyromagnetic ratio.
correct
incorrect
15
N due to its low natural abundance and small gyromagnetic ratio.
correct
incorrect
13
C due to its low natural abundance and small gyromagnetic ratio.
correct
incorrect
31
P due to its high natural abundance and large gyromagnetic ratio.
correct
incorrect
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not completed
.
Cross-polarisation build-up curves can be used to
probe distances between and the mobility of spins due to the dependence of cross-polarisation build-up on spin mobility.
correct
incorrect
probe distances between and mobility of spins due to the dependence of cross-polarisation build-up on spin relaxation.
correct
incorrect
probe distances between and mobility of spins since spin relaxation is independent of spin mobility.
correct
incorrect
probe distances between and mobility of spins due to a dependence of spin relaxation on spin mobility and separation.
correct
incorrect
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not completed
.
Incomplete averaging of quadrupolar interactions during magic angle spinning
can provide useful information about the structure and mobility by analysis of the isotropic chemical shift.
correct
incorrect
can provide useful information about structure and mobility through analysis of the quadrupolar lineshape.
correct
incorrect
can provide useful information about structure through analysis of the chemical shift anisotropy.
correct
incorrect
does not provide any information beyond line broadening.
correct
incorrect
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