Nuclear Physics Flashcards

1
Q

What are 3 interpretation of results of particle scattering experiment?

A
  1. most particles pass thru undeflected/ w small deflect n
    - since vv few particle scattered thru large angles, prob of particle getting close to centre of +ve charge small
    => atom cosist of mostly empty space
  2. small fraction (<1%) of α-particle deflected thru large angle
    - to produce large deflect n, must hv large force
    - all +ve charge in atom concentrated as nucleus in small region of space vs diameter of atom
  3. few particles reflected backwards, thru angle close to 180 deg
    - nucleus is vv small, massive (vv large mass in small space)
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2
Q

Give order of magnitude of nuclear and atomic diameters

A
  • nuclear: ~10E-15 m
  • atomic: ~10E-10 m
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3
Q

Define proton/atomic number, nucleon/mass number

A
  • proton/atomic no. , Z, give no. of proton in nucleus
  • nucleon/mass no. , A, give total no. nucleons (proton + neutron) in nucleus, A=Z+N
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4
Q

Describe nuclide notation

A
  • notat n for nucleus X, atomic no. Z, mass no. A is
    A
    X
    Z
  • a nuclide is a particular species w unique pair values A, Z. It is represented by notat n above where X is chem symbol of element
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5
Q

Define isotope

A

atoms w same no. proton but diff no. of neutron

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6
Q

Name some common isotopes

A
  • H: hydrogen, deuterium, tritium
  • C: carbon-12, carbon-14
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7
Q

Define unified atomic mass unit

A
  • one unified atomic mass unit is 1/12 mass of carbon-12 atom
    thus,

1u = 1.66E-27 kg

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8
Q

Define relative atomic mass, m r

A

m r is of atom is ratio of mass of atom to unified atomic mass unit

m r = mass of atom / 1/12 mass of carbon-12 atom

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9
Q

Describe mass-energy equivalence

A

mass can b ‘created’ or destroyed’; when this happen, equivalent amt energy simultaneously vanish or come into being. Energy E produced by change of mass m is given by mass-energy equivalence relat n:
E = mc²

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10
Q

Define electron-volt (Nuclear Physics)

A

1 electron-volt is energy gained by charge equal to that of e- in moving thru pd of 1 volt

1eV = 1.60E-19J

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11
Q

Define mass defect of a nucleus. What is the formula?

A

diff btw mass of separated nucleon & combined mass of nucleus

Δm = sum of m (nucleons) - m (nucleus)
* if u calculate mass defect of ATOM,

Δm = sum of m (nucleons+e-) - m nucleus

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12
Q

Define binding energy (BE). What is the formula?

A

nuclear BE of nucleus is min energy to completely separate nucleus into constituent neutron, proton

BE = Δmc²

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13
Q

Explain important feature of graph of BE/nucleon against mass number

A
  • high rate +ve graph that bcome gentler until ard Fe, then gently -ve graph

impt feature:
- except for lighter nuclei, avg BE/nucleon abt 8MeV
- Fe nucleus located close to peak w BE/nucleon ~ 8.8MeV, one of most stable nuclide that exist
- nuclei w vv low, high mass no. hv lower BE/nucleon & less stable
- nuclei w low mass no. located to left side of peak may undergo nuclear fusion, so final pdt may hv greater BE/nucleon (more stable)
- nuclei w high mass no. located to right of peak may undergo nuclear fission to form daughter nuclei w greater BE/nucleon

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14
Q

Define nuclear fission

A

disintegrat n of heavy nucleus into 2 lighter nuclei of approx equal mass

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15
Q

Define nuclear fusion

A

combining of 2 light nuclei to produce heavier nucleus

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16
Q

What are conserved in all nuclear processes?

A
  • nucleon no.
  • proton no. (Charge)
  • linear momentum
  • mass-energy (same both sides)
17
Q

Describe some problems of nuclear reactors

A
  • disposal of radioactive fission fragments
  • accidental release of highly radioactive fission fragments into atmos
18
Q

Define radioactive decay. Elaborate

A
  • spontaneous emis n particles (α, β particle) and/or radiat n (gamma ray) fr unstable nucleus so that it bcome more stable
  • radioactive decay is spontaneous & random
  • spontaneous bcos not affected by external condit n (eg physical factor eg Pa, temp, B, E-fields)
  • random bcos impossible predict which nucleus decay next. There is const prob that nucleus decay in any fixed period of time
19
Q

Explain evidence of randomness of radioactive decay

A
  • random nature of radioactive decay can b determined by observe fluctuat n in count rate
  • when Geiger-Muller (GM) tube is near radioactive source, irregularity of counts & fluctuat n in count rate recorded by GM tube show randomness of radioactive decay

NOTE: GM tube is a device to measure count rate (& hence activity) of radioactive source

20
Q

What are the types of radiation (Nuclear Physics)?

A
  • alpha particle
  • beta particle
  • gamma ray
21
Q

Explain alpha particles

A
  • helium-4 nuclei
  • typically hv energy in range of few MeV
  • speed of order 10^7
  • deflected by strong B field (being +ve charge)
  • oso deflected by e- field
  • high ionising pwr (can remove e- fr nearby species effectively), produce large no. of ion along path
  • range in air abt 3-4cm, easily stopped by piece of paper
  • cause substance eg zinc sulfide to fluoresce, blacken photographic plate
22
Q

Explain beta particles

A
  • high speed e-, emitted when neutron in nucleus decay into proton
  • emitted w range of speeds, can travel up to 50% light speed
  • pdt of beta decay process cnt just consist daughter nuclide & beta particle as no definite speed for both pdt for linear momentum b conserved
  • oso observed that daughter nuclide no recoil back in straight line but at angle
  • by conserv n law energy, momentum, there must b 3rd particle produced in process
    => neutrino (mass-less, charge-less, so hard to detect)
  • easily deflected by B, e-field (so low mass)
  • ionising pwr abt 1/10 of alpha particle (so lower charge)
  • range of beta particles in air abt 10 times that of alpha particle; stopped oni by few mm thick Al
23
Q

Explain gamma rays

A
  • EM waves (shorter wavelength than X ray)
  • electrically neutral, not deflected by e-, B field
  • strongest penetrate pwr, stopped by lead of few cm thick
  • ionisat n pwr abt 1/10 000 of alpha particle
  • emis n no accompany any change in nuclear structure; nucleus just descend to lower energy state
  • gamma decay represent emis n energy fr nucleus returning to ground state

excited nucleus -> more stable nucleus + gamma ray

24
Q

Define decay constant of nucleus

A

nucleus’ probability of decay per unit time

25
Q

Give equations involving decay constant, activity and count rate

A

N = N0e^(-λt) OR N = N0(0.5)^n

A = A0e^(-λt) OR A = A0(0.5)^n

A = -dN/dt = λN

C = C0e^(-λt) OR C = C0(0.5)^n

where
N is no. of radioactive nuclide,
A is activity (rate decay parent nuclei),
C is corrected count rate (detected decay),
0 is initial value,
λ is decay const,
t is time taken,
n is no. of half lives passed

26
Q

Define activity of radioactive source

A

no. of nuclear decay per unit time occurring in source

27
Q

Describe graphical representation of decay of parent nuclide

A
  • N vs t graph give decrease exponential graph
    N = N0e^(-λt)
  • ln N vs t graph give w grad -ve straight line graph
    ln N = lnN0 -λt
28
Q

Describe cancer treatment with radiation

A
  • amt irradiat n used in each treatment of patient usually same
    => for freshly prepared sample, durat n of treatment is shorter
  • if same sample used later, durat n of treatment is longer for patient to receive same dose

Since, amt radiat n (dose) = At, can form
A1t1 = A2t2 to find new duration of treatment

29
Q

Define half-life (nuclear physics)

A

time taken for half og no. of radioactive nuclei to decay

30
Q

Explain background radiation

A
  • to determine measuremt of rad n fr radioactive scs, we must consider backgrd rad n (ionising rad n emitted fr variety of natural, artificial rad n scs)
  • backgrd rad n come fr environ ard us, present in small amt
  • lvl of rad n vary fr place to place
  • accidents at nuclear pwr station or any form of nuclear dumping cause increase backgrd rad n
  • backgrd rad n come fr scs eg,
    air (cosmic ray), building material, soil (+ rock containing radioactive isotope), water, human body, old coal fired pwr station, medical scs)
31
Q

Explain effects of radiation on living organisms

A
  • hazards to human beings arise fr: exposure of body to external rad n & ingest n/inhalat n of radioactive matter
  • alpha particle: slight hazard (unless enter body) since cnt penetrate outer layer of skin
  • beta particle: generally more penetrating than alpha; most of their energy absorbed by surface tissues, few mm of Al suff to provide protect n
  • gamma ray: highly penetrating; can penetrate deeply into body, may require few cm lead or concrete shielding
  • rad n can cause immediate severe damage to body tissue eg rad n burn, by damage structure of molecules, cause malfunct n, death of living cells (some cell recover but others cnt, effect on tissues r cumulative)
  • delayed effects eg cancer, eye cataract may appear many yr later
  • hereditary defects may oso occur in succeeding gen due to genetic damage
  • chromosome r sensitive to ionising rad n at moment of cell divis n causing genetic mutat n likely harmful; such can cause birth defect if unborn child &/or mother exposed
32
Q

Name and explain uses of radiation

A
  1. tracers
    - used to follow path of cpd thru system
    eg leak in undergrd pipe carrying water, oil can b detected by inject radioactive tracer into flow
    - geiger tube on surface r then used to detect leakage
  2. medical, biological uses
    - immature cell, cell growing/dividing most rapidly r most sensitive to rad n; this is made use of in rad n treatmt of cancer
    - often, cancer cell growing rapidly, so more likely killed by high dose gamma rad n fr cobalt-60 scs vs normal cell dividing less frequently
  3. Archaeological dating (carbon dating)
    - atmos contain small proport n radioactive carbon-14, absorbed by living plant, trees during photosynthesis
    - half-life of C-14 is 5700 yr, so there is negligible disintegrat n over lifetime of most plant
    - BUT, once plant dies, no further carbon-14 is taken in, so proport n of carbon-14 in plant starts decrease as it decay
    - after 1 half-life, 50% of carbon-14 remain
    - since activity is proportional to no. of C-14 atom left, measuring activity enable age (time since death) of dead sample to b calculated)
    - measured activity is compared w activity of same mass of living wood, then using value of half-life of C-14, age can b determined (up to abt 20 000 yr limit)
33
Q

Explain safety precautions for radiation

A
  1. handling
    - minimise time contact w radioactive material
    - solid scs most easily handled, shd b manipulated remotely fr dist eg use tong, in glove-box, etc
    - avoid any ingest n eg radioactive particles lodged in lungs much more danger, harmful than outside body
    - rad n worker given protective clothing, regular test monitor dosage they receive
    - limit amt rad n received fr X-ray equipmt
  2. storage
    - penetrating pwr of diff type rad n give clue to safe practice; pure alpha particle present little hazard when enclosed in container; but since most alpha scs oso emit gamma rad n, lead-lined container needed. same is true for beta scs
    - generally, keep all radioactive material in lead container when not in use
  3. disposal
    - radioactive waste pdt must b quickly, safely disposed of; they can b encased in concrete, sealed in steel tanks, then buried undergrd