Bloch–McConnell equations
E646669
The Bloch–McConnell equations are an extension of the Bloch equations that describe nuclear magnetic resonance (NMR) signal evolution in systems with chemical exchange between different spin populations.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Bloch–McConnell equations canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T7145248 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Bloch–McConnell equations Context triple: [Bloch equations, relatedTo, Bloch–McConnell equations]
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A.
Bloch–Torrey equation
The Bloch–Torrey equation is an extension of the Bloch equations that incorporates diffusion effects to describe the evolution of nuclear magnetization in magnetic resonance imaging and NMR.
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B.
Bloch equations
The Bloch equations are a set of differential equations in nuclear magnetic resonance and quantum mechanics that describe the time evolution of nuclear magnetization in an external magnetic field.
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C.
Karplus equation for NMR coupling constants
The Karplus equation for NMR coupling constants is an empirical relationship that links three-bond scalar coupling values between nuclei to the dihedral angle between them, enabling the determination of molecular conformations from NMR data.
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D.
Bhabha–Corben equations
The Bhabha–Corben equations are relativistic wave equations in quantum electrodynamics that describe the dynamics of spinning charged particles, developed by physicists Homi J. Bhabha and H. C. Corben.
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E.
Wiener–Hopf equations
Wiener–Hopf equations are integral equations that arise in problems of filtering, prediction, and diffraction, forming the mathematical foundation for optimal linear filters such as the Wiener filter.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Bloch–McConnell equations Target entity description: The Bloch–McConnell equations are an extension of the Bloch equations that describe nuclear magnetic resonance (NMR) signal evolution in systems with chemical exchange between different spin populations.
-
A.
Bloch–Torrey equation
The Bloch–Torrey equation is an extension of the Bloch equations that incorporates diffusion effects to describe the evolution of nuclear magnetization in magnetic resonance imaging and NMR.
-
B.
Bloch equations
The Bloch equations are a set of differential equations in nuclear magnetic resonance and quantum mechanics that describe the time evolution of nuclear magnetization in an external magnetic field.
-
C.
Karplus equation for NMR coupling constants
The Karplus equation for NMR coupling constants is an empirical relationship that links three-bond scalar coupling values between nuclei to the dihedral angle between them, enabling the determination of molecular conformations from NMR data.
-
D.
Bhabha–Corben equations
The Bhabha–Corben equations are relativistic wave equations in quantum electrodynamics that describe the dynamics of spinning charged particles, developed by physicists Homi J. Bhabha and H. C. Corben.
-
E.
Wiener–Hopf equations
Wiener–Hopf equations are integral equations that arise in problems of filtering, prediction, and diffraction, forming the mathematical foundation for optimal linear filters such as the Wiener filter.
- F. None of above. chosen
Statements (50)
| Predicate | Object |
|---|---|
| instanceOf |
NMR theory
ⓘ
mathematical model ⓘ system of differential equations ⓘ |
| appliesTo |
multi-pool magnetization models
ⓘ
multiple spin populations ⓘ systems with chemical exchange ⓘ two-pool magnetization models ⓘ |
| assumes | first-order chemical exchange kinetics ⓘ |
| basedOn | Bloch equations formalism NERFINISHED ⓘ |
| characteristic |
coupled differential equations for each exchanging site
ⓘ
matrix representation of magnetization and exchange ⓘ |
| describes |
NMR signal evolution
ⓘ
chemical exchange between spin populations ⓘ exchange broadening of NMR lines ⓘ magnetization dynamics in exchanging systems ⓘ multi-site chemical exchange ⓘ relaxation in exchanging spin systems ⓘ two-site chemical exchange ⓘ |
| domain | theoretical NMR spectroscopy ⓘ |
| extends | Bloch equations NERFINISHED ⓘ |
| field |
chemical physics
ⓘ
magnetic resonance imaging ⓘ magnetic resonance spectroscopy ⓘ nuclear magnetic resonance ⓘ physical chemistry ⓘ spin dynamics ⓘ |
| includes |
chemical exchange rate constants
ⓘ
longitudinal relaxation terms ⓘ off-diagonal exchange terms in the magnetization matrix ⓘ transverse relaxation terms ⓘ |
| language | mathematics ⓘ |
| namedAfter |
Felix Bloch
NERFINISHED
ⓘ
Harden M. McConnell NERFINISHED ⓘ |
| relatedTo |
Bloch equations
NERFINISHED
ⓘ
Bloch–Torrey equations NERFINISHED ⓘ Redfield theory NERFINISHED ⓘ |
| relates |
observed NMR line shapes to exchange rates
ⓘ
observed relaxation to exchange processes ⓘ |
| usedFor |
analysis of saturation transfer experiments
ⓘ
chemical exchange saturation transfer (CEST) modeling ⓘ dynamic NMR studies ⓘ exchange spectroscopy (EXSY) analysis ⓘ interpretation of NMR line shapes ⓘ magnetization transfer contrast modeling ⓘ quantitative analysis of exchange rates ⓘ |
| usedIn |
biomolecular NMR
ⓘ
in vivo spectroscopy ⓘ magnetic resonance imaging research ⓘ solid-state NMR ⓘ solution-state NMR ⓘ |
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Subject: Bloch–McConnell equations Description of subject: The Bloch–McConnell equations are an extension of the Bloch equations that describe nuclear magnetic resonance (NMR) signal evolution in systems with chemical exchange between different spin populations.
Referenced by (1)
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