Magnets and Scanner Flashcards

Mriquestions.com

1
Q

What imparts magnetic characterics to all materials?

A

Angular momenta of electrons (and to a lesser extent, nuclei) impart some magnetic characteristics to all materials.

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2
Q

What generates a magnetic field?

A

Any current, moving charge, or changing electrical potential also generates a magnetic field.

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3
Q

What is the today’s understanding of the magnetism? Today we understand that the static magnetic fields associated with lodestones and permanent magnets derive principally from the ____ within those materials.

A

Today we understand that the static magnetic fields associated with lodestones and permanent magnets derive principally from the total angular momentum of electrons within those materials.

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4
Q

What is spin?

A

Possessed by lone electrons; quantized fundamental property of nature denoted by the letter S.

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5
Q

In addition to spin, what does electrons orbiting a nucleus possess?

A

In addition to S, electrons orbiting a nucleus also possess orbital angular momentum (L).

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6
Q

Total Angular Momentum

A

Spin + Orbital Angular Momentum

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7
Q

Who first demonstrated the relationship between current and strength of the resultant magnetic field?

A

Andre Marie Ampere

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8
Q

Who demonstrated principle of magnetic induction?

A

Michael Faraday

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9
Q

How did Faraday demonstrate principle of magnetic induction?

A

Not only do electrical currents produce magnetic fields, but changing magnetic fields induce electrical currents. By measruing the voltage produced in a coil by a moving magnet.

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10
Q

Three years after Faraday demonstrated the principle of magnetic induction, who showed that the current induced was so directed as to oppose the change in magnetic flux?

A

Heinrich Lenz

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11
Q

emf = -N(delta magnetic flux / delta time)

A

Lenz’s Law represents the rate change of the magnetic field. The negative sign reflects Lenz’s principle that the induced current creates a “counter field” in a direction opposite to magnetic field(B).

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12
Q

Maxwell’s Four Equations in words

A

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

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13
Q

Maxwell’s four equations in order mean: 1) ; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

A

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

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14
Q

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) ; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

A

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

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15
Q

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) 4) either a constant current or changing electric field creates a circulating magnetic field.

A

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

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16
Q

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4)

A

Maxwell’s four equations in order mean: 1) wherever a charge exists, an electric field E diverges from it or into it; 2) magnetic field lines (B) can only exist in closed loops; 3) an electric field (E) is produced by a changing magnetic field (dB/dt) and 4) either a constant current or changing electric field creates a circulating magnetic field.

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17
Q

What is Tesla?

A

SI unit of magnetic field strength

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18
Q

How is Tesla Defined?

A

Force per unit length exerted on a current-carrying wire

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19
Q

1 Tesla =

A

1 Newton / Ampere-Meter

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20
Q

When a current is passed along the wire, a magnetically generated (Lorentz) force

A

When a current is passed along this wire, a magnetically generated (Lorentz) force deflects the wire upward.

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21
Q

Lorentz Force is proportional to the current(I), The length of the wire(L), Strength of the magnetic field(B)

A

F = i * L * B

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22
Q

In general, however, the structure of the magnetic field is more complex, and B may have –

A

In general, however, the structure of the magnetic field is more complex, and B may have different values and directions of action at different points in space.

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23
Q

A magnetic field is therefore formally defined to be an __ (denoted by the boldfaced letter B) whose magnitude B and direction at each point in space define how the field will act on a charge moving at that location.

A

A magnetic field is therefore formally defined to be an array of vectors (denoted by the boldfaced letter B) whose magnitude B and direction at each point in space define how the field will act on a charge moving at that location.

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24
Q

Vector Form of Lorentz Force Law

A

F = I x B

25
Q

Relationship between Gauss and Tesla

A

1T = 10,000 Gauss

26
Q

Relative Magnetic Field Strength
Earth, Refrigerator Magnet

A

Earth : 50 uT, Refrigerator Magnet: 5 mT

27
Q

How is Gradient Defined?

A

Gradient(G) is defined as change in field over a change in distance

28
Q

When does a magnetic gradient exist?

A

Whenever a magnetic field differs in magnitude or direction between

29
Q

The main magnetic field, the gradient (G) is a vector, possessing both magnitude and direction. By convention, the direction of the main magnetic field is designated to be —-. For completeness, therefore, we should say the gradient (G) is a vector of magnitude 2 mT/meter in the z-direction.

A

Note we have calculated only the magnitude of the gradient. But like the main magnetic field, the gradient (G) is a vector, possessing both magnitude and direction. By convention, the direction of the main magnetic field is designated to be the z-axis. For completeness, therefore, we should say the gradient (G) is a vector of magnitude 2 mT/meter in the z-direction.

30
Q

The gradient of B is denoted ∇B, where ∇ is known as the “—” operator. Because B is a vector, ∇B is a Jacobian or 2nd order tensor, a matrix of 9 partial derivatives of the 3 principal components of B (Bx, By, and Bz) with respect to the 3 cardinal directions (x, y, and z).

A

The gradient of B is denoted ∇B, where ∇ is known as the “del” operator. Because B is a vector, ∇B is a Jacobian or 2nd order tensor, a matrix of 9 partial derivatives of the 3 principal components of B (Bx, By, and Bz) with respect to the 3 cardinal directions (x, y, and z).

31
Q

Fortunately, in MR imaging, we can often assume relatively simplified cases like the one above. For example, the x-, y- and z-gradients used for imaging are generally considered to create variations of B only with respect to the —- component. Thus as a good first order approximation, we need only consider the partial derivatives in the third column of the Jacobian, assuming all —-.

A

Fortunately, in MR imaging, we can often assume relatively simplified cases like the one above. For example, the x-, y- and z-gradients used for imaging are generally considered to create variations of B only with respect to the Bz component. Thus as a good first order approximation, we need only consider the partial derivatives in the third column of the Jacobian, assuming all derivatives in the first two columns are zero.

32
Q

Isn’t a gradient some type of coil?

A

Gradient Coils produce the gradient fields. gradient describes how a magnetic field changes in space. An ideal, uniform magnetic field in a vacuum contains no gradients

33
Q

gradient describes how a magnetic field changes in space. An ideal, uniform magnetic field in a vacuum contains no gradients. However, all real-life MR magnets have gradients due to field imperfections (—). Additionally, any object in the scanner (e.g., the human body) interacts with and distorts the field, an effect called —–.

A

gradient describes how a magnetic field changes in space. An ideal, uniform magnetic field in a vacuum contains no gradients. However, all real-life MR magnets have gradients due to field imperfections (inhomogeneities). Additionally, any object in the scanner (e.g., the human body) interacts with and distorts the field, an effect called susceptibility.

34
Q

gradient is used synonymously with gradient coils, a set of electromagnets embedded in the body of the MR magnet assembly. When an electrical current is passed through these coils, the main magnetic field is focally distorted in certain places, creating magnetic gradients of the first kind. Gradient coils alter the main magnetic field in a — manner in the x-, y-, and z-directions and are used to —- the MR signal

A

gradient is used synonymously with gradient coils, a set of electromagnets embedded in the body of the MR magnet assembly. When an electrical current is passed through these coils, the main magnetic field is focally distorted in certain places, creating magnetic gradients of the first kind. Gradient coils alter the main magnetic field in a predictable manner in the x-, y-, and z-directions and are used to spatially encode the MR signal

35
Q

What is Susceptibility?

A

Susceptibility is a measure of the extent to which a substance becomes magnetized when it is placed in an external magnetic field. A synonym for susceptibility is “magnetizability”.

36
Q

When matter interacts with the magnetic field, an — is created that either opposes or augments the external field.

A

When matter interacts with the magnetic field, an internal magnetization or polarization (J) is created that either opposes or augments the external field.

37
Q

What is diamagnetism?

A

If the polarization opposes the applied field, the effective field within the object is reduced, the lines are dispersed

38
Q

How to calculate magnetic susceptibility?

A

Magnitude of Internal Polarization(J) / Strength of an external magnetic field(Bo)

39
Q

What is the dimension of magnetic susceptibility?

A

Since it is the ratio of two magnetic fields, susceptibility is a dimensionless number.
Internal Magnetization / Polarization(J)

40
Q

What kinds of substances have negative susceptibilities?

A

Diamagnetic substances have negative susceptibilities (χ < 0); paramagnetic, superparamagnetic, and ferromagnetic substances have positive susceptibilities (χ > 0).

41
Q

What kinds of substances have positive susceptibilities?

A

Diamagnetic substances have negative susceptibilities (χ < 0); paramagnetic, superparamagnetic, and ferromagnetic substances have positive susceptibilities (χ > 0).

42
Q

What kinds of magnetism does biological tissues have?

A

Nearly all biological tissues are weakly diamagnetic.

43
Q

Nearly all biological tissues are weakly diamagnetic. However, some can be paramagnetic. Why?

A

Some tissues contain focal accumulations of metals such as iron, gadolinium, copper, or manganese that concentrate the magnetic field and are therefore paramagnetic.

44
Q

Nearly all biological tissues are weakly diamagnetic. However, some can be Superparamagnetic. Why?

A

A few tissues also contain chunky iron-based protein conglomerates (ferritin and hemosiderin) that are superparmagnetic

45
Q

Are there ferromagnetic substances in our body?

A

Other than trace amounts of magnetite that do not contribute to bulk susceptibility, there are no endogenous ferromagnetic substances in the human body.

46
Q

If there are no ferromagnetic susbtances in our body, why do we have to be careful in MRI?

A

many extrinsic metallic foreign bodies and surgical implants are ferromagnetic, and these are commonly encountered in MR imaging

47
Q

What causes susceptibility?

A

Susceptibility is caused by interactions of electrons and nuclei with the externally applied magnetic field.

48
Q

Please explain paramagnetism in terms of spins

A

When nuclear and electron spins in a material orient in the same direction as the magnetic field, their individual magnetic moments locally augment the field. This augmentation of the external field is called paramagnetism.

49
Q

What do you call magnetic effects opposing the applied field?

A

Diamagnetism.

50
Q

What determines the overall magnetic susceptibility of a material?

A

Electrons are much smaller than nuclei, so we can think of their spins being as being “concentrated” into smaller volumes. As a consequence of this spin/size discrepancy, electron-field interactions are thousands of times stronger than nuclear ones. Electrons, not nuclei, primarily determine overall magnetic susceptibility of a material.

51
Q

Expalin why orbitals are important in magnetism.

A

In addition to having spin, electrons “orbit” the nucleus and possess a second quantum property - orbital angular momentum (L). How electrons are distributed among orbitals is critical in determining magnetic susceptibility. Orbitals containing paired electrons contribute to diamagnetism; orbitals with unpaired electrons contribute to paramagnetism.

52
Q

In most substances there are several competing diamagnetic and paramagnetic effects whose net sum determines bulk susceptibility. The major mechanisms contributing to susceptibility are briefly described below. Give me a list.

A

Langevin (Larmor) diamagnetism.
Van Vleck paramagnetism.
Nuclear paramagnetism.
Curie Paramagnetism.
Mechanisms in simple metals (Pauli Paramagnetism and Landau Diamagnetism).
Exchange Coupling and Magnetic Domains.

53
Q

What causes Langevin(Larmor) Diamagnetism?

A

Results from Angular momentum (L) of electrons in filled orbitals. Through a quantum process similar to Lenz’ Law, the orbital motion of paired electrons generates an internal field that opposes the externally applied one. The effect is relatively weak, but because all molecules contain at least some filled orbitals, Langevin diamagnetism is present in all materials. Langevin diamagnetism dictates the overall susceptibility of a material unless it is overridden by a more powerful mechanism.
Water, most biological materials, nonmetallic atoms, stable salts, and covalently bonded molecules have no unpaired electrons, so their overall susceptibilities are dominated by Langevin diamagnetism. Their susceptibilities (χ) are weak and negative, typically with values close to −0.00001.

54
Q

Is Langevin Diamagnetism present in all materials?

A

Yes. Results from Angular momentum (L) of electrons in filled orbitals. Through a quantum process similar to Lenz’ Law, the orbital motion of paired electrons generates an internal field that opposes the externally applied one. The effect is relatively weak, but because all molecules contain at least some filled orbitals, Langevin diamagnetism is present in all materials. Langevin diamagnetism dictates the overall susceptibility of a material unless it is overridden by a more powerful mechanism.

55
Q

Which materials are dominated by Langevin Diamagnetism?

A

Water, most biological materials, nonmetallic atoms, stable salts, and covalently bonded molecules have no unpaired electrons, so their overall susceptibilities are dominated by Langevin diamagnetism. Their susceptibilities (χ) are weak and negative, typically with values close to −0.00001.

56
Q

Explain what Van Vleck Paramagnetism is.

A

Van Vleck paramagnetism. This can be considered a minor counter-effect to Langevin diamagnetism, becoming important only for a few polyatomic molecules and certain atoms/ions with shells exactly one electron short of being half-filled. In water, for example, Van Vleck paramagnetism is only 10% the strength of Langevin diamagnetism.

57
Q

What effect can be considered a minor counter effect to Langevin Diamagnetism?

A

Van Vleck Paramagnetism. Important only for a few polyatomic molecules and certain atoms or ions with shells exactly one electron short of being half filled. In water, Van Vleck paramagnetism is only 10% the strength of Langevin Diamagnetism.

58
Q
A