Chapter 40 Flashcards

(31 cards)

1
Q

Electron Transitions (photon radiation)

A
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2
Q

Pauli Exclusion Principle

A
  1. A very important physics principle forbids any two electrons to occupy the same quantum state. This is called the Pauli principle.
  2. Each electron must occupy a unique state defined by a unique set of quantum numbers:
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3
Q

Why does orbitals do not fill up in the expected order according to energy levels

A

This is because (for example) the 3𝑑^6 4𝑠^2 configuration results in a lower energy state for the atom than 3𝑑^8

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4
Q

Total energy of an electron on shell n:

A
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5
Q

When doesnt this equation apply

A

For 𝑍>1, because of electron shielding.

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6
Q

For 𝑍>1 what equation do we use to calulate energy in electron shell

A
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7
Q

The effective charge is equal to the

A

atomic number (all the protons) minus the shielding effect, 𝑆.
𝑄=π‘βˆ’π‘†

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8
Q

K_𝛼 electron transitions energy of the emitted photon is given by:

A
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9
Q

𝐿_𝛼 transitions the energy of the emitted photon is given by:

A
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10
Q

Electron tranistion summary

A
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11
Q

Electron tranistion summary

A
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12
Q

Moseley Equation

A
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13
Q

Moseley Equation

A
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14
Q

Three possible ways to obtain EM radiation from atoms

A
  1. Excitation β†’ De-excitation of electrons
  2. Knock an electron out of orbit
  3. Bremsstrahlung
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15
Q

Excitation β†’ De-excitation of electrons

A

shine light on the material, or heat the material, thereby causing the electrons to jump to higher energy levels. Once the energy source is removed, the electrons will de-excite (they always seek to be in the lowest energy state) and emit radiation/photons

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16
Q

Knock an electron out of orbit

A

direct a beam of electrons at an atom. Some electrons will be knocked out of orbit, leaving β€œholes”. Electrons in higher energy levels will move to these lower energy levels (they always seek to be in the lowest energy state) and emit radiation/photons.

17
Q

Brehmsstrahlung

A

An accelerating electron emits radiation (Larmor Radiation)

When an electron approaches the negatively charged β€œelectron cloud” of an atom it slows down (it brakes!). During this deceleration it emits radiation

Therefore:
1. Small acceleration β‡’ low energy radiation
2. Large acceleration β‡’ high energy radiation

18
Q

literally thousands of applications:

A

Laser cutters (e.g. cuts car frames)
Fibre optics
CD/DVD player
Sensitive measuring devices

19
Q

Why are lasers so useful

A
  1. Monochromatic
  2. Coherent
  3. Directional
20
Q

Three important processes of lasers

A
  1. Absorbtion
  2. Spontaneous emission
  3. Stimulated Emission:
21
Q

Three important processes of lasers

A
  1. Absorbtion
  2. Spontaneous emission
  3. Stimulated Emission:
22
Q

absorbtion

A

electron absorbs a photon and β€œjumps up” to an excited state.

23
Q

Spontaneous emission

A

Electron spontaneously de-excites, and releases a photon

24
Q

Spontaneous emission

A

Electron spontaneously de-excites, and releases a photon

25
Stimulated Emission:
Electron de-excites as a result of a stimulus. The stimulus is an external photon. This is weird! It is a similar process to β€œabsorbtion”, but the electron de-excites
26
Stimulated Emission:
Electron de-excites as a result of a stimulus. The stimulus is an external photon. This is weird! It is a similar process to β€œabsorbtion”, but the electron de-excites
27
types of atomic transitions
28
Lifetime of electrons
When one (or more) electron(s) are not in their lowest possible energy state, we say that an atom is in an excited state. We don’t know when a particular electron will de-excite. In other words, the lifetime of the excited state of a particular atom cannot be predicted
29
equation to find out how many atoms are in excited state
If 𝑁_0 is the number of atoms in an excited state at 𝑑=0, then at some time, 𝑑, later we have 𝑁(𝑑)=𝑁_0 𝑒^((βˆ’πœ†π‘‘) ) atoms in an excited state. Different atoms (e.g. 𝐻, 𝐻𝑒, 𝐿𝑖) have different lifetimes; i.e. different decay constants πœ†
30
Half life
The time it takes for half of a large collection of atoms to de-excite to their ground state
31
Derviving half life equation