All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a proton, has an
value of ½ and two possible orientations. The orientation aligned with the field (called spin +½, spin-up, or α) has lower energy than the orientation aligned against the field (called spin −½, spin-down, or β).
From Chapter 7:
Now Playing
Principles of Nuclear Magnetic Resonance
1.0K Views
Principles of Nuclear Magnetic Resonance
2.0K Views
Principles of Nuclear Magnetic Resonance
1.6K Views
Principles of Nuclear Magnetic Resonance
843 Views
Principles of Nuclear Magnetic Resonance
911 Views
Principles of Nuclear Magnetic Resonance
1.1K Views
Principles of Nuclear Magnetic Resonance
602 Views
Principles of Nuclear Magnetic Resonance
598 Views
Principles of Nuclear Magnetic Resonance
237 Views
Principles of Nuclear Magnetic Resonance
1.0K Views
Principles of Nuclear Magnetic Resonance
721 Views
Principles of Nuclear Magnetic Resonance
649 Views
Principles of Nuclear Magnetic Resonance
804 Views
Copyright © 2025 MyJoVE Corporation. All rights reserved