Jbguptaelectricalengineeringpdfdownload __LINK__

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Published: September 5, 2022 (3 weeks ago)
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Jbguptaelectricalengineeringpdfdownload __LINK__



 
 
 
 
 
 
 

Jbguptaelectricalengineeringpdfdownload

jbguptaelectricalengineeringpdfdownload
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I’ve been living in London, off and on, since the 2006. all on all devices. Laptop with Windows 8.1 Pro.
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A nuclear magnetic resonance (NMR) system includes a magnet for creating a static magnetic field (B0) and a radio frequency (RF) coil for creating an RF magnetic field (B1) orthogonal to the B0 field. A subject, typically a human patient, is typically located inside the B0 and B1 field of the NMR system. Nuclei of interest within the subject, such as Hydrogen-1 (H-1) protons, and nuclei of interest outside the subject, such as Nitrogen-13 (N-13) or Carbon-13 (C-13) protons, provide signals for the NMR system. Various sequences of B0 and B1 magnetic fields are applied to the subject to affect nuclear magnetic relaxation and thus encode the NMR signals from the desired nuclei. A key parameter for good NMR signal acquisition is the “T1” (time constant) of protons within the subject, which is the reciprocal of the proton spin-lattice relaxation time. The “T1” of protons in the subject is dependent on many factors, including temperature and the proton-imaging pulse sequence, among others.
For a proton imaged at an arbitrary location within the subject, there is a phase ambiguity due to the phase-encoding orientation. The phase can be unambiguously identified only by knowing the direction in which the phase was created and thus knowing the location of the proton of interest within the subject. Unfortunately, in most cases, the orientation of the B1 field is not known due to the spatially non-uniform B1 field. As a result, the proton of interest is encoded into undesired locations, resulting in inaccurate image reconstruction.
It is possible to correct the B1 field orientation by applying a series of RF pulses, each with different RF phases. The location of a proton of interest is encoded into a specific phase based on the location of the phase. The location of the proton of interest is subsequently decoded from the phase based on the known history of the applied RF pulses. Unfortunately, the phase-encoding orientation is based on a “target” location of the proton. Unfortunately, it is not always known where the proton of interest is within the subject, making it impossible to determine the correct phase.
It is desirable to have a method and system of acquiring NMR signals that correct the undesired encoding of the NMR signal

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