Lectures 1&2 (Basics, FM & Bohr-van Leeuwen) Flashcards

(36 cards)

1
Q

What is magnetisation?

A

Response of a material due to an applied magnetic field

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2
Q

Flux density inside solenoid?

A

B = µ0 IN/L

(so H = IN/L)

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3
Q

Magnetic moment equation?

A

µ = MV

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4
Q

µ units?

A

Am^2

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5
Q

Angular momentum equation for an electron?

A

l = m_e * r x v

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6
Q

How is M defined?

A

Magnetic moment per unit volume

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7
Q

Show that magnetic moment µ can be given in terms of the angular momentum l of the electron

A

l = m_e * r x v

and µ = -e/2 * r x v

µ = - e/2m * l

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8
Q

Equation for µ in terms of orbital angular momentum?

A

µ = γl

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9
Q

γ value?

A

γ = -e/2m or -ge/2m for > 1 electron

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10
Q

Show that Bohr magneton comes from magnetic moment and orbital angular momentum

A

µ = -e/2m * l

µ_z = -e/2m * m_l * ℏ

µ_B = eℏ/2m

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11
Q

Show that µ = µ0(1+X)

A

B = µ0(H+M) = µ0(H+XH) = µ0H(1+X) = µH

where µ = µ0(1+X)

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12
Q

Which materials experience diamagnetism?

A

All

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13
Q

Susceptibility of a diamagnet?

A

X < 0

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14
Q

How do diamagnets react to magnetic fields?

A

Weakly repelled

(A small opposite moment is induced due to Lenz’s law)

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15
Q

What gradient does a diamagnet have on the M vs H graph?

A

-ve

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16
Q

Susceptibility of a paramagnet?

17
Q

How do paramagnets react to magnetic fields?

A

Weakly attracted

Moments not aligned in absence of H_ext

18
Q

Which materials experience paramagnetism?

A

Those with net angular momentum on each atom

19
Q

Why does a FM remain magnetised at H=0?

A

Exchange interaction and anisotropy

20
Q

X of FM?

A

X_eff = ∂M/∂H

21
Q

What is Ms?

A

Magnetisation of the sample when all domains are aligned and characteristic of the material

22
Q

What is Mr?

A

Remanent magnetisation is that at zero field, and can depend on the sample

23
Q

What is Hc?

A

The coercive field (coercivity) is the reverse field that needs to be applied to zero magnetisation

24
Q

What is Mr/Ms?

A

Remanent fraction / loop squareness

25
What is work density in a hysteresis loop?
µ0 ∫M.dH = energy lost in the material by going around the loop
26
Spin and orbital magnetic moment equations?
µ_z,l = -e/2m * m_l * ℏ µ_z,s = -e/m * m_s * ℏ
27
What does a skinny hysteresis loop mean?
Less energy lost
28
Why is Permalloy good for magnetic recording?
Easily magnetisable (soft)
29
What properties are good for permanent magnets?
High Ms and large Hc
30
Are Ms, Hc and Mr sample independent?
Only Ms
31
Does Ms depend on T?
Yes
32
When does Ms vanish?
At Tc - above which material becomes paramagnetic
33
What does the Bohr-van Leeuwen theorem show?
According to classical physics, there is no interaction between an applied field and the electrons in a material
34
Brief steps to show the BvL theorem?
(Model material as system of charges. Check affect of H as to whether M induced) Electron energy: E = -µ.B = -µ.µ0H = -µBcosø But m. field means Lorentz force F = q(E + vxB) - so the B always produces forces perp. to the velocity No work is done by the magnetic field, so there is no change in energy So µ ~ E/B doesn't depend on m. field
35
How can exchange energy be estimated?
kTc
36
Why is there a discrepancy form g=2?
Because interactions are due to virtual photons. Electrons emit and reabsorb virtual photons if µ is measured during the lifetime of a virtual photon there is an extra orbital component