Principles of the MRI Signal Contrast Mechanisms MR

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 ﺍﻟﻄﺒﻴﺔ ﺍﻟﻔﻴﺰﻳﺎﺀ ﻣﺤﺎﺿﺮﺍﺕ Principles of the MRI Signal Contrast Mechanisms MR Image Formation

ﺍﻟﻄﺒﻴﺔ ﺍﻟﻔﻴﺰﻳﺎﺀ ﻣﺤﺎﺿﺮﺍﺕ Principles of the MRI Signal Contrast Mechanisms MR Image Formation

How do protons interact with a magnetic field? • Moving (spinning) charged particle generates

How do protons interact with a magnetic field? • Moving (spinning) charged particle generates its own little magnetic field – Such particles will tend to line up with external magnetic field lines (think of iron filings around a magnet) • Spinning particles with mass have angular momentum – Angular momentum resists attempts to change the spin orientation (think of a gyroscope)

index Interaction with B 0 1. Orientation :

index Interaction with B 0 1. Orientation :

index Interaction with B 0 2. Energy states : DE = għBo = ħwo

index Interaction with B 0 2. Energy states : DE = għBo = ħwo

index Interaction with B 0 3. Precession : Rotation or precession about the axis

index Interaction with B 0 3. Precession : Rotation or precession about the axis of the magnetic field Bo with frequency : wo = g. Bo wo = Larmor frequency g = gyromagnetic ratio

index Interaction with B 0 3. Precession : At the equilibrium state : -

index Interaction with B 0 3. Precession : At the equilibrium state : - rotation in phase - no transverse magnetization Mxy y x

Effect of Static Field on Protons Bo

Effect of Static Field on Protons Bo

index Interaction with B 0 4. Summary : at the equilibrium state : 1.

index Interaction with B 0 4. Summary : at the equilibrium state : 1. spin orientation « up » > « down » longitudinal magnetization Mz 2. precession no transverse magnetization Mxy

Interaction with B 1 Resonance phenomenon TRANSITIONS Transitions E 1 E 2 Mz decreases

Interaction with B 1 Resonance phenomenon TRANSITIONS Transitions E 1 E 2 Mz decreases REPHASING Phase coherence increases Mxy increases !!! RF frequency = Larmor frequency = w 0 !!!

index Interaction with B 1 From the macroscopic point of view… Two different processes

index Interaction with B 1 From the macroscopic point of view… Two different processes : 1. Transitions E 1 E 2 Mz decreases 2. Rephasing Mxy increases The macroscopic magnetization flips from the z-axis to the xy-plane and precesses

Precession in Magnetic Field

Precession in Magnetic Field

Net magnetization

Net magnetization

Net magnetization • Small B 0 produces small net magnetization M • Larger B

Net magnetization • Small B 0 produces small net magnetization M • Larger B 0 produces larger net magnetization M, lined up with B 0 • Thermal motions try to randomize alignment of proton magnets • At room temperature, the population ratio of antiparallel versus parallel protons is roughly 100, 000 to 100, 006 per Tesla of B 0

The Zeeman effect n The dependence of electronic transition energies on the presence of

The Zeeman effect n The dependence of electronic transition energies on the presence of a magnetic field reveals electron spin (orbital angular momentum)

Energy Difference Between States

Energy Difference Between States

Energy Difference Between States D E = h n D E = 2 mz

Energy Difference Between States D E = h n D E = 2 mz B o n = g/2 p Bo known as Larmor frequency g/2 p = 42. 57 MHz / Tesla for proton Knowing the energy difference allows us to use electromagnetic waves with appropriate energy level to irradiate the spin system so that some spins at lower energy level can absorb right amount of energy to “flip” to higher energy level.

Basic Quantum Mechanics Theory of MR Spin System Before Irradiation Bo Lower Energy Higher

Basic Quantum Mechanics Theory of MR Spin System Before Irradiation Bo Lower Energy Higher Energy

The Effect of Irradiation to the Spin System Lower Higher

The Effect of Irradiation to the Spin System Lower Higher

Basic Quantum Mechanics Theory of MR Spin System After Irradiation

Basic Quantum Mechanics Theory of MR Spin System After Irradiation