Calcium-Binding Protein Protocols Calcium-Binding Protein Protocols

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Calcium-43 NMR 217 18 Calcium-43 NMR of Calcium-Binding Proteins Torbjörn Drakenberg 1. Introduction The Ca 2+ -ion, with its closed-shell electronic structure, has very few spectroscopic properties that are useful in studies of calcium-binding proteins and their interactions with calcium ions. Therefore, it is even more important to exploit the few possibilities for spectroscopy that are available. The most abundant calcium isotope, 42 Ca, has a spin quantum number I = 0 and is therefore not observable by NMR. However, 43 Ca has I = 7/2 and is in principle NMR active. The natural abundance of this istope is only 0.15% and 43 Ca NMR can therefore most likely never be used to study biological systems without isotope enrichment. Nowadays, 43 Ca enriched to 50% is readily available, though at a rather high cost. It seems that most research groups working with calciumbinding proteins consider the 43 Ca isotope as an exotic one and only a limited number of groups have been involved in 43 Ca NMR studies of biological systems (1–6). Only the Swedish group in Lund and the Japanese group in Sendai have been using 43 Ca NMR more consistently. Below I will first present, very briefly, what is special about the application of 43 Ca NMR as compared to typical spin = 1/2 nuclei like 1 H, 13 C, and 15 N and than discuss some typical studies. 2. Experimental and Theoretical Considerations Because 43 Ca is a quadrupolar nucleus with a quite high spin quantum number (I = 7/2) it has properties that are in some respects different from the dipolar nuclei that are mostly considered in studies of macromolecules. From an experimental point of view it is essential to recognize that sensitivity is the most important fact to consider because the natural width of the 43 Ca NMR resonance from a 43 Ca 2+ ion bound to a macromolecule is hundreds, if not thou- From: Methods in Molecular Biology, vol. 173: Calcium-Binding Protein Protocols, Vol. 2: Methods and Techniques Edited by: H. J. Vogel © Humana Press Inc., Totowa, NJ 217
218 Drakenberg sands, of Hertz broad. In a way that should simplify the life for the experimentalist because he does not have to compromise between sensitivity and resolution. On the other hand, there seem to be no probes for this purpose available from the NMR vendors. Even if a high sensitivity probe is available, spectra have to be accumulated for a long time, often more than 10 5 transients. This puts high demands on the “ring-down time” of the probe. The specifications by the vendors provide no guidance on this. They have most likely never had to run a 1D spectrum with one million transients. The simple remedy for this problem of course would be to increase the dead time, i.e., the time between the end of the last pulse and the acquisition of the first data point, until there is no effect from probe ringing. Unfortunately, for 43 Ca NMR, this has most likely also removed the signal you want to observe. A better way is therefore to use the so-called RIDE sequence (7) to minimize the effect from probe ringing. This has worked quite well in our hands and made the observation of resonances that are approx 1000 Hz broad possible even for as much as 10 6 transients. The basic theory for NMR may be found in standard text books for NMR (see, e.g., Ernst, Bodehausen, and Wokaun [8]) and will not be presented here. Some aspects particular for quadrulopar nuclei that will be of importance for the following discussion will be dealt with here. NMR spectra of quadrupolar nuclei like 43 Ca will be dominated by the effects of the quadrupole moment. In this chapter, I will consider only isotropic solutions, and furthermore limit myself to present only the effects on the linewidth (relaxation) and not on the chemical shift, because such effects have not yet been observed for 43 Ca even though they can be foreseen. In isotropic solutions the linewidth of the 43 Ca resonance will be dominated by the quadrulopar relaxation mechanism and is determined by the quadrupole coupling constant, χ = e 2 qQ, and the correlation time τ c. Only when the extreme narrowing condition applies (ω 0τ c
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Methods in Molecular BiologyTM Biol
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M E T H O D S I N M O L E C U L A R
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© 2002 Humana Press Inc. 999 River
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Preface Calcium plays an important
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Contents Dedication ...............
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Contents xi 26 Enzymatic Assays to
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xiv Contents of Companion Volume 15
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xvi Contributors LESLIE D. HICKS
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20 Dean, Kelsey, and Re
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2 Yazawa
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4 Yazawa Fig. 1. Schematic represen
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6 Yazawa Fig. 2. Shop drawing for t
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8 Yazawa DuPont-NEN and the molar c
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10 Yazawa Fig. 4. Examples of the C
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12 Yazawa 5. Plot the calculated Ca
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14 Yazawa 12. Starovasnik, M. A., D
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16 Fig. 1. Molecular structures and
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18 Linse 7. 0.1 M EDTA. Dissolve 37
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20 Linse iterate the other paramete
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22 Linse tive to small alterations
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24 Linse References 1. Tsien, R. Y.
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26 Haiech and Kilhoffer to use the
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28 Haiech and Kilhoffer where γ is
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30 Haiech and Kilhoffer reporter gr
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32 Haiech and Kilhoffer tein with i
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34 Haiech and Kilhoffer Calmodulin
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36 Haiech and Kilhoffer Fig. 3. Mec
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38 Haiech and Kilhoffer We may sugg
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40 Haiech and Kilhoffer 29. Stewart
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42 Haiech and Kilhoffer 62. Becking
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44 Martin and Bayley Fig. 1. Absorp
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46 Martin and Bayley evaporation. C
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48 Martin and Bayley 4. Set the tem
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50 Martin and Bayley Fig. 2. Near-U
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52 Martin and Bayley discussed by M
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54 Martin and Bayley References 1.
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20 Dean, Kelsey, and Reik
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58 Fabian and Vogel are equipped wi
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60 Fabian and Vogel The penetration
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62 Fabian and Vogel perature, ionic
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64 Fabian and Vogel Fig. 3. IR spec
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66 Fabian and Vogel Fig. 4. Lower t
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68 Fabian and Vogel These correlati
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70 Fabian and Vogel Fig. 5. Amide I
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72 Fabian and Vogel 4. ATR-FTIR spe
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74 Fabian and Vogel 25. Georg, H.,
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76 Weljie and Vogel Fig. 1. Simplif
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78 Weljie and Vogel Fig. 3. Steady-
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80 Weljie and Vogel VIS spectrophot
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82 Weljie and Vogel 4. A series of
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84 Table 1 Advanced Fluorescence Me
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86 Weljie and Vogel References 1. L
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90 Johnson and Tikunova is removed
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92 Johnson and Tikunova function of
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94 Johnson and Tikunova Fig. 2. Rat
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96 Johnson and Tikunova Fig. 3. Rat
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98 Johnson and Tikunova Fig. 4. Ca
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100 Johnson and Tikunova cence inte
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102 Johnson and Tikunova 6. Johnson
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104 Julenius Fig. 1. Under conditio
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106 Julenius 3. Mix 50 µL of NHS s
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108 Julenius Fig. 3. A typical sens
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110 Julenius (2), is used in the Ia
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114 Lopez and Makhatadze Fig. 1. Th
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116 Lopez and Makhatadze 6. Buffers
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118 Lopez and Makhatadze The excess
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122 Lopez and Makhatadze Fig. 1. Is
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124 Lopez and Makhatadze 2.5 mL are
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126 Lopez and Makhatadze pendence o
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128 Hicks et al. equipped with a pu
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130 Hicks et al. Fig. 2. Debye plot
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132 Hicks et al. and 1.0 mg/mL for
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134 Hicks et al. Fig. 3. Sedimentat
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136 Hicks et al. 5. Hayes, D. B. (M
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138 Trewhella and Krueger This chap
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140 Trewhella and Krueger of the sc
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142 Trewhella and Krueger Table 1 C
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144 Trewhella and Krueger beam, or
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146 Trewhella and Krueger At very l
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148 Trewhella and Krueger analytica
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150 Trewhella and Krueger collapsed
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152 Trewhella and Krueger P(r) func
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154 Trewhella and Krueger Fig. 3. S
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156 Trewhella and Krueger concentra
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158 Trewhella and Krueger by a Nati
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162 Doherty-Kirby and Lajoie metal
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164 Doherty-Kirby and Lajoie two Ca
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Page 227 and 228: 208 Clarke and Vogel Fig. 1. 113 Cd
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Page 275 and 276: 256 Li et al. In order for these ex
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268 Mal et al. NMR data, X-PLOR (11
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270 Mal et al. Table 1 Simulated An
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272 Mal et al. 3.1.2.1. AMBIGUOUS D
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274 Mal et al. molecular dynamics a
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276 Mal et al. Assuming a rigid bod
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278 Mal et al. assign (segid A and
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280 Mal et al. References 1. Drenth
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282 Mal et al. 33. Jeener, J., Meie
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286 Werner et al. Our research has
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288 Fig. 1. (A) T 1, T 2 and the he
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290 Werner et al. tion, using gradi
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292 Werner et al. Fig. 3. (A) Rotat
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294 Werner et al. Fig. 4. (A) Line-
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296 Werner et al. Table 2 Models of
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298 Werner et al. 9. Reinhardt, D.
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300 Werner et al. 39. Press, W. H.,
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302 Boyd et al. utilize residual di
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304 Boyd et al. Fig. 1. (A) The sol
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306 Boyd et al. or significant peak
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308 Boyd et al. Fig. 3. Histogram o
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310 Boyd et al. total and NOE energ
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312 Boyd et al. 2. When studying mu
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314 Boyd et al. 4. Downing, A. K.,
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316 Boyd et al. 35. Schulte-Herbrug
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318 Yap et al. image representation
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320 Yap et al. modified EF-hand is
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322 Table 1 Angle and Distance Outp
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324 Yap et al. 2. Ikura, M. (1995)
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326 Kobayashi that S-100A1 and S-10
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328 Kobayashi 3.2. Coupling of Crom
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330 Kobayashi Fig. 2. Tricine/SDS/P
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332 Kobayashi 0.1% TFA at a flow ra
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334 Kobayashi Both recombinant S-10
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336 Kobayashi Fig. 6. Affinity chro
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340 Walsh et al. verts CaM from an
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342 Walsh et al. 11. Bovine serum a
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344 Walsh et al. Fig. 1. CaM-depend
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348 Walsh et al. 3.5. NOS Reduction
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354 Walsh et al. 3. Cho, M. J., Vag
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356 Hughes et al. The electroporati
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358 Hughes et al. 4. 1 M Na 2CO 3.
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360 Hughes et al. range, repeat ste
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362 Hughes et al. Table 1 Examples
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366 Persechini of the different CaM
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368 Persechini Fig. 1. Schematic re
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370 Persechini 2. 1 L of Terrific b
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372 Persechini Fig. 4. Titration wi
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374 Persechini Table 1 Parameters f
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376 Persechini Fig. 6. The [Ca 2+ -
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378 Persechini determined if the di
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380 Persechini relatively insensiti
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382 Persechini 18. Chafouleas, J. G
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384 Török et al. actions in the c
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386 Török et al. 3. The reaction
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388 Török et al. Fig. 2. Electros
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390 Török et al. Fig. 3. Peptides
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392 Török et al. Table 1 Peptide
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394 Török et al. Fig. 7. Nanospra
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396 Török et al. Fig. 9. Nanospra
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398 Török et al. Fig. 11. Electro
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400 Török et al. 3 µM FL-calmodu
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402 Török et al. Fig. 14. Localiz
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404 Török et al. Fig. 16. Indicat
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406 Török et al. the significantl
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408 Török et al.
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410 Index substitutes, see Fluoresc
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412 Index Stern-Volmer plot, 78, 81
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414 Index Phenothiazines, see Calmo
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