8.3 - Nuclear Instability & Radius Flashcards

1
Q

What are more stable, lighter or heavier elements?

A

Lighter.
Z < 20

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2
Q

What are 4 things that will make a nucleus unstable?

A
  • too many neutrons
  • too many protons
  • too many nucleons
  • too much energy
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3
Q

On an N against Z graph, what proves the sample is an alpha emitter?

A
  • Occur beneath the line of stability when Z > 60 (too many nucleons)
  • Number of protons > number of neutrons
  • strong force between nucleons is unable to overcome the electrostatic force of repulsion between the protons
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4
Q

On an N against Z graph, what proves the sample is a beta-minus emitter?

A
  • Occur to the left of the stability line where isotopes are neutron-rich
  • Neutron is converted to a proton
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5
Q

On an N against Z graph, what proves the sample is a beta-plus emitter?

A
  • Occur to the right of the stability line where the isotopes are proton-rich
  • Proton is converted to a neutron
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6
Q

On an N against Z graph, what proves the sample undergoes electron capture?

A
  • When a nucleus captures one pf its own orbiting electrons
  • occurs to the right of the stability line - proton-rich
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7
Q

What is a nuclear excited state?

A

When an unstable nucleus decays, it may emit remaining energy in the form of a gamma photon. (does not change number of nucleons, just a release of energy)

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8
Q

What is technetium-99m used for? (and what does the m stand for)

A
  • Used as a gamma source in medical diagnoses
  • The m stands for metastable - nucleus exists in a particularly stable excited state
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9
Q

What are nuclear energy levels?

A

The nucleus, like the atom, has discrete energy levels whose location and properties are governed by the rules of quantum mechanics.

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10
Q

When does alpha emission occur?

A

When there are TOO MANY NUCLEONS in a nucleus.
- too large to be stable as the strong nuclear force between the nucleons is unable to overcome the electrostatic force of repulsion between the protons.

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11
Q

When does Beta-minus emission occur?

A
  • When an atom is neutron rich.
  • neutron decays into a proton (+ anti-electron neutrino)
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12
Q

When does Beta-plus emission occur?

A
  • When an atom is proton rich.
  • proton decays into neutron (+ electron neutrino)
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13
Q

When does electron capture occur?

A
  • When a nucleus captures one of its own orbiting electrons
  • a proton in the nucleus is converted into a neutrino, releasing a gamma-ray (+ electron neutrino)
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14
Q

If a nucleus has too much energy, what does it emit?

A

Gamma rays.
(often happens after alpha/beta decay as the nucleus often has excess energy)

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15
Q

What does Beta minus emission look like on an N/Z graph?

A

N - 1
Z + 1
So graphically it will go down to the right diagonally.

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16
Q

What does Beta plus emission look like on an N/Z graph?

A

N +1
Z - 1
So graphically it will go up and to the left diagonally.

17
Q

What does alpha emission look like on an N/Z graph?

A

N - 2
Z - 2
So graphically it goes down and to the left by 2 squares

18
Q

What does gamma emission look like on an N/Z graph?

A

There is no change to the nuclear constituents in gamma emission as its just letting out energy.

19
Q

How does a nucleus exist in an excited state?

A

It’s the same as electrons. A system is given additional energy and this causes it to move to an excited state for a short amount of time.

20
Q

What does the energy level diagram for nuclear reactions look like for alpha decay of uranium?

A

(Search it up). It moves diagonally to the bottom right.

21
Q

What are the 2 methods to measure the nuclear radius?

A
  • rutherford scattering (the closest approach method)
  • electron scattering
22
Q

How is Rutherford scattering used to measure the nuclear radius?

A
  • initial kinetic energy of alpha particle = max electric potential energy (closest approach)
  • initial Ek = Qq/4πε0r
    q = 2e (ALPHA PARTICLE)
    Q = 79e (GOLD)

This can then be rearranged for the radius

23
Q

What does the Rutherford scattering experiment show us about the atom’s structure?

A
  • There must be a positive nucleus as there electrostatic repulsion between the nucleus and alpha particle - (some alpha particles are deflected at great angles)
  • atom must be mostly empty space as lots of alpha particles move straight through the gold foil
24
Q

What is the typical value for a nuclear radius?

A

1fm (1 x 10^-15)

25
Q

What are 3 advantages of the closest approach method?

A
  • good estimate of the upper limit for a nuclear radius
  • maths simple
  • alpha particles only scatter by protons (not nucleons).
26
Q

What are 4 disadvantages to the closest approach method?

A

Always an overestimate of radius (as it measures the smallest separation not the radius):
- does not account for strong nuclear force effects
- gold nucleus recoils as alpha particle approaches
- very few alpha particles rebound at exactly 180 degrees.

27
Q

How does electron diffraction estimate the nuclear radius?

A
  • A beam of electrons are directs at a nucleus (thin foil) and they diffract around it
  • the pattern formed by this diffraction has a predictable minimum which forms at an angle X to the original direction according to the equation
    sinX = λ /d
    sinX = angle of the first minimum
    λ = de broglie wavelength (h/mv)
    d = size of the nucleus
28
Q

Where is the first minimum of electron diffraction pattern? (after beam of electrons if fired at thin foil)

A

sinX = 1.22λ /2R

29
Q

What are is the advantage of electron scattering?

A
  • electron scattering is much more accurate than closest approach (as strong nuclear force is not in play)
30
Q

What are 2 disadvantages of electron scattering?

A
  • electrons must be accelerated to very high speeds to maximise the resolution
    (this is because significant diffraction takes place when the electron wavelength is similar to size of nucleus (λ ∝ 1/v) )
  • electrons can be scattered by both protons and neutrons - excessive scattering, difficult to determine first minima
31
Q

How does intensity vary with angle in electron scattering?

A

intensity of the maxima decreases as the angle of diffraction increases.

32
Q

What is the nuclear radius proportional to?

A

The cube root of the nucleon number

33
Q

What is the equation to show the relationship between the nuclear radius and the nucleon number?

A

R = R₀A¹/³
R = nuclear radius
A = nucleon/mass number
R₀ = constant of proportionality = 1.05fm

34
Q

Make the equation for the relationship between nuclear radius and nucleon number into a straight line graph?

A

lnR = ln(R₀A¹/³)
lnR = lnR₀ + lnA¹/³
lnR = lnR₀ + 1/3lnA
y = c + mx
m = 1/3
y = lnR
x = lnA
c = lnR₀

35
Q

what is the mass of the nucleus equal to?

A

m = Au
A = mass number
u = atomic mass unit - 1u = 1.661x10^-27

36
Q

How can you prove that all nuclei have a similar density?

A

p = m/v = A x m(of nucleon) / 4/3πR³ = A x m(of nucleon / 4/3π(R₀A¹/³)³ = 3m(of nucleon)/ 4πR₀³ = constant

37
Q

What is the density of a nucleus?

A

p = 3u/4πR₀³