Bloch equations
E166545
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.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Bloch equations canonical | 4 |
| Rabi formula for magnetic resonance | 1 |
| optical Bloch equations | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T1455589 — 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 equations Context triple: [Felix Bloch, notableWork, Bloch equations]
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A.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
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B.
London equations
The London equations are fundamental relations in superconductivity that describe how magnetic fields behave inside superconductors, capturing key features like the Meissner effect and zero electrical resistance.
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C.
Maxwell's equations
Maxwell's equations are the fundamental set of four equations in classical electromagnetism that describe how electric and magnetic fields are generated and interact with charges and currents.
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D.
Faraday effect
The Faraday effect is a magneto-optical phenomenon in which the polarization plane of light is rotated as it passes through a material under the influence of a magnetic field aligned with the direction of propagation.
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E.
Tomonaga–Schwinger equation
The Tomonaga–Schwinger equation is a relativistic generalization of the Schrödinger equation that formulates quantum field evolution on arbitrary spacelike hypersurfaces, forming a key part of covariant quantum field theory.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Bloch equations Target entity description: 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.
-
A.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
-
B.
London equations
The London equations are fundamental relations in superconductivity that describe how magnetic fields behave inside superconductors, capturing key features like the Meissner effect and zero electrical resistance.
-
C.
Maxwell's equations
Maxwell's equations are the fundamental set of four equations in classical electromagnetism that describe how electric and magnetic fields are generated and interact with charges and currents.
-
D.
Faraday effect
The Faraday effect is a magneto-optical phenomenon in which the polarization plane of light is rotated as it passes through a material under the influence of a magnetic field aligned with the direction of propagation.
-
E.
Tomonaga–Schwinger equation
The Tomonaga–Schwinger equation is a relativistic generalization of the Schrödinger equation that formulates quantum field evolution on arbitrary spacelike hypersurfaces, forming a key part of covariant quantum field theory.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
physical law
ⓘ
set of differential equations ⓘ |
| appliesTo |
electron spins
ⓘ
nuclear spins ⓘ |
| assumes |
classical description of spin precession
ⓘ
macroscopic magnetization approximation ⓘ phenomenological relaxation ⓘ |
| coordinateSystem |
laboratory frame
ⓘ
rotating frame ⓘ |
| describes |
dynamics of spin systems in magnetic fields
ⓘ
time evolution of nuclear magnetization ⓘ |
| developedBy | Felix Bloch ⓘ |
| domain | continuous time ⓘ |
| field |
nuclear magnetic resonance
ⓘ
quantum mechanics ⓘ |
| governs | magnetization vector M ⓘ |
| hasComponent |
longitudinal relaxation term
ⓘ
precession term ⓘ transverse relaxation term ⓘ |
| hasSolutionType |
exponential relaxation
ⓘ
sinusoidal precession ⓘ |
| includesParameter |
T1 relaxation time
ⓘ
T2 relaxation time ⓘ equilibrium magnetization ⓘ |
| includesVariable |
Mx component of magnetization
ⓘ
My component of magnetization ⓘ Mz component of magnetization ⓘ gyromagnetic ratio γ ⓘ magnetic field B ⓘ |
| influenced | development of NMR-based imaging techniques ⓘ |
| involves | cross product of magnetization and magnetic field ⓘ |
| mathematicalForm | first-order linear differential equations ⓘ |
| relatedTo |
Bloch–McConnell equations
ⓘ
Bloch–Torrey equation ⓘ Liouville–von Neumann equation ⓘ |
| usedFor |
analysis of relaxation processes
ⓘ
description of free induction decay ⓘ modeling of spin echo formation ⓘ simulation of NMR experiments ⓘ |
| usedIn |
electron spin resonance
ⓘ
magnetic resonance imaging ⓘ magnetic resonance pulse sequence design ⓘ nuclear magnetic resonance spectroscopy ⓘ |
| usesConcept |
Larmor precession
ⓘ
external magnetic field ⓘ magnetization vector ⓘ relaxation times ⓘ |
| yearProposed | 1946 ⓘ |
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Subject: Bloch equations Description of subject: 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.
Referenced by (6)
Full triples — surface form annotated when it differs from this entity's canonical label.