The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated. Concept introduction: Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z − axis, with no x − and no y − component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

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Answer 1

Question

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

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Answer 2

Question

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

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Answer 3

Question

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

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Answer 4

Question

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

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Answer 5

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

Answer 6

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

Answer 7

Chapter 12, Problem 12C.2BE

Interpretation Introduction

Interpretation:

The effective transverse relaxation time when the width of a Lorentzian resonance line is 12 Hz has to be calculated.

Concept introduction:

Relaxation is the process by which the magnetization returns to its equilibrium value, at which point it is entirely along the z− axis, with no x− and no y− component (no transverse components). In practice, due to the limitations in the design of the magnet, the field is not perfectly uniform and is different at different locations in the sample. The inhomogeneity results in an inhomogeneous broadening of the resonance. the extent of inhomogeneous broadening is expressed in terms of transverse relaxation time.

Answer 8

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Answer 9

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Answer 10

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Answer 11

Ch. 12 - Prob. 12B.1ST Ch. 12 - Prob. 12B.2ST Ch. 12 - Prob. 12B.3ST Ch. 12 - Prob. 12D.1ST Ch. 12 - Prob. 12A.1DQ Ch. 12 - Prob. 12A.2DQ Ch. 12 - Prob. 12A.3DQ Ch. 12 - Prob. 12A.1AE Ch. 12 - Prob. 12A.1BE Ch. 12 - Prob. 12A.2AE

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