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A one-dimensional (1D) NMR spectrum of a protein HNHN HH Chemical shifts in parts per million (ppm)...
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Transcript of A one-dimensional (1D) NMR spectrum of a protein HNHN HH Chemical shifts in parts per million (ppm)...
![Page 1: A one-dimensional (1D) NMR spectrum of a protein HNHN HH Chemical shifts in parts per million (ppm) Are independent of the field strength of the Static.](https://reader035.fdocuments.us/reader035/viewer/2022062802/56649ea45503460f94ba8ed2/html5/thumbnails/1.jpg)
A one-dimensional (1D) NMR spectrum of a protein
CO N
HΝ
Cα CO
Hα
HN Hα
€
Ω(HN)
€
Ω(Hα )
€
Ωref
€
δ ( )ppm=(Ω− Ωref )/Ωref
Chemical shifts in parts per million (ppm)Are independent of the field strength of theStatic magnetic Bo field.
See the supplementary lecture material andRattle, ‘NMR Primer for Life ScientistsPages 19-21, 26.
9
Backbone HN
Aromatics
H2O
Hα
Upfield shiftedmethyls
Methyl
8 7 6 5 4 3 2 1 0
1H chemical shift (ppm)
600.134800 600.132400600.130000
For a 1H protein spectrum we need a fair amount of protein, maybe 5-10 mgs of protein. 600 L sample volume - gives a 1-2 mM concentration of protein.
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The 1D 1H spectrum of a protein
0123456789ppm
Amides
Aromatics
H2O
CαH
CH
CH CδH
Upfield shiftedmethyl
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A lot of work done with histidine since the C2 proton appears at higherfrequency than most other protons.
C
H
COO-+H3N
C
C
NC
N
C
HH
H
+1
2
3
4
H H
H6.8-7.2 ppm
8.0-8.8 ppm
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1H NMR spectrum of Histidine - C2 proton appears at higher frequency than most other protons and is sensitive to the protonation of the ring.
C2H C4H CαH CH
010
Raise pH
10 0ppm
8.0-8.8 ppm
6.8-7.2 ppm
C
H
COO-+H3N
C
C
NC
N
C
HH
H
+1
2
3
4
H H
H
Shown in protonated form
α
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pH1 3 5 7 9 11
ChemicalShiftChangeδ ppm)
0
1
Titration of the C2H of Histidine
pKa = 5.2
Shift measured with multiple 1D spectra starting withpH 1.0 and moving through to pH 9
The chemical shift change of the proton on C2 reflects the protonation of N1
50% ofcomplete change
C
H
COO-+H3N
C
C
NC
N
C
HH
H
+1
2
3
4
H H
H
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4 histidines which couldbe monitored and have their pKa’s measured.
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H1 = His105H2 = His119H3 = His12H4 = His48
Measure pKa of each histidine
pKa
His105 6.7
His119 6.2
His12 5.8
His48 is more complex,sudden discontinuity in thecurve.
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Found that 200mM Na+CH3COO-
helped to stabilize the protein.
Can then determine that the pKaof C2H is 6.31.
There is a conformational change affecting this peak so that at some pHs two peaks were observed. H4a and H4b were acid and basestable forms.
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His105
His12
His48
His119His48 and His105 are unchanged
His12 and His119 curved are shifteddownfield.
Why downfield??
His119 changes from 6.2 to 8.0His 12 changes from 5.8 to 7.4
Both His12 and His119 are protonated in the enzyme-inhibitor complex. The proton is protected from exchange by the presence of the inhibitor. Need to go to higher pH to remove it.
Repeat titrations in the presenceof an inhibitor.
in this case, cytidine-3’-monophosphate (3’-CMP) O
OPO3- OH
NHOCH2
NH2
O
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O
OPO3- OH
NHOCH2
NH2
O
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A simple 1D NMR Spectrum - this is ethanol but the spectrum has the sort of simplicity we might get with a one amino acid protein(there is no such thing!)
A 36 amino acid proteinA successful NMR experiment comes in 3 stages,
1.) Resolve the resonances - that is, obtain a spectrumwhere individual signals are clearly resolved from oneanother.
2.) Assign the resonances. Each peak comes from oneatom in the protein - but which one? Our 36 amino acidprotein is a mess! The record to date is 723 amino acidsWith full assignment of the spectrum - how did they dothis?
3.) Interpret the data.
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Effect of increasing spectrometer frequency
1 GHz soon??
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13
rad s-1
rad s-1 T-1. T
€
ωo
2π= vo
vo =γBo
2π
s-1 (Hz)
Larmor Frequency
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14
A compass in a magnetic field
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15
A nuclear spin precesses in a magnetic field
the circulating motion of the spin angular momentum is called precession
Nuclear spins precess because:• they are magnetic•they have angular momentum
this arrow denotes the direction of the spin angular momentum
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16
Precession frequency = Larmor frequency0 = - Bo/2π
Larmor frequency in Hz (= cycles per second)
gyromagnetic ratio in rad s–1 T–1
magnetic field inTesla (T)
€
E = γhBo
ΔE = hωo
ωo = γBo
Compare with Zeeman Splitting
€
,Since ωo = 2πvo
ωo = −γBo
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x
y
zBo
€
ωo = −γBo
α
Magnetic vectors precess around the static magnetic field at thelarmor frequency. There is a slight population excess in the low energy (α) state. This leads to a net magnetization along Z (in green). There is no net magnetisationalong x or y as this is essentially randomised.
x
y
α
x
y
α
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Generation of transverse magnetization by π/2 pulse
x
y
z
(/2)x
x
y
z
/2
Magnetization perpendicular to the magnetic field is called transverse
magnetization
yNet Moment
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NMR signal
Note the orientation of the coil -perpendicular to the magnetic field x
y
z Bo
Preamp
The NMR signal is also called the free induction decay
(fid)
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Precession of Transverse Magnetization
The transverse magnetization components oscillate and decay
Mx
My
Time
Time
x
y
z
x
y
z
x
y
zBo
xy plane
My (t) = -Mzeq cos(ωt) exp{-t / T2}
Mx (t) = Mzeq sin(ωt) exp{-t / T2}
oscillation at the Larmor frequency
decay time constant = spin-spin relaxation time OR transverse relaxation time
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Pg 46 & 47 of Rattle
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Diagonal
DiagonalCrosspeaks
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COSY of Alanine in D2O
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COSY Spectrum of a small protein
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Areas of Spectrum
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Typical Amino Acid spin-system patterns on COSY spectra
1.) Just see 3Jcoupling
2.) Do notsee couplingsacross the peptide bond.
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