Nucleus Flashcards
Size of nucleus
R = RoA1/3
Ro = 1.2 x 10-15 m
A1/3 = mass no.
Density of nucleus
2.2 x 1017 kg/m3
SAME FOR ALL NUCLEI
1 amu - definition + relation to kg
1 amu is (1/12)th of the mass of a C-12 atom
1 u = 1.66 x 10-27 kg
Classification of nuclei
- Isotopes
- Isobars
- Isotones
Isotopes w examples
Same no. of protons (Z)
Different no. of neutrons
so A and A-Z is different
E.g. 1H1 , 2H1 , 3H1
16O8 , 17O8 , 18O8
Isobars with examples
Same no. of nucleons (A)
Different no. of protons/atomic no (Z)
Different no. of netrons (A-Z)
E.g.3H1 , 3He2
Isotones w examples
Different mass no. (A)
Different no of protons/atomic no (Z)
Same no. of neutrons (A-Z)
E.g.7Li3 , 8Be4
What particles are released in alpha decay
4He2
Particles released in Beta decay
β+ decay : 0β1 (positron) + 𝜈 (neutrino)
β- decay : 0β-1 (electron) + anti-neutrino
Gamma decay particle
𝜈 - neutrino
excited state to ground state
mass defect
difference between mass of protons and neutrons in free state and mass of nucleus
Δm formula
Δm = [Z(mp) + (A-Z)mn - M]
where Z= at. no.
mp = mass of proton
A = Mass no.
mn = mass of neutron
M = mass of nucleus
Binding energy
Minimum energy required to separate the nucleons of nucleus and place them at rest at infinite distance apart
BE = Δmc2
=[Z(mp) + (A-Z)mn - M]c2
=[Z(mp) + (A-Z)mn - M] * 931.5 MeV
as 1u * c^2 = 931.5 MeV
BE curve bw mass no. A = 50 to A = 80
- The curve has almost a flat maximum roughly from A = 50 to A = 80 corresponding to an average binding energy / nucleon of about 8.5 MeV
- Fe56 has the highest BE / nucleon of 8.76 MeV
BE curve A>80
- Average BE / nucleon decreases slowly and drops to about 7.6 MeV for uranium (A = 238)
- Unstable nuclei, beyong Bismuth (A=209), they are radioactive
- Undergo nuclear fission to reduce mass no.
BE curve A<50
- Less stable
- Have the tendency to fuse together because BE is less (nuclear fusion) ==> to increase mass no. so that BE increases
- Even nuclei have larger BE than neighbouring nuclei E.g. C12 and O16
Nuclear fission
Process in which a heavy nucleus after capturing a thermal neutron splits into two lighter nuclei of comparable masses
What is used in nuclear bombs and nuclear reactors: nuclear fusion or nuclear fission
Nuclear fission
Explain chain reaction of nuclear fission
- When a uranium (92U235) nucleus is bombarded by a slow neutron, the nucleus is split into two nearly equal fragments along with emission of energy and two or three fast neutrons.
- Under favourable conditions, the emitted nuetrons collide with other uranium nuclei nearby in the same manner causing further emission of energy and more neutrons
- Thus, a chain reaction of nuclear fissions is established until the whole of the uranium is consumed
- About 200 MeV is emitted per fission
How can chain reaction be maintained in natural uranium despite the small concentration of 92U235
- With the help of moderators, by slowing down the emitted neutrons to thermal neutrons
- The probability of these neutrons getting absorbed by 92U238 and fissioning 92U235 increases
- E.g. graphite and heavy water
Uncontrolled chain reaction
In an uncontrolled chain reaction, the reaction occurs rapidly so that the energy is released instantaneously and therefore, we can’t convert any of that into any useful form of energy.
E.g. nuclear bomb
Controlled chain reaction
If the reaction is controlled in such a way that only one of the neutrons emitted in a fission causes another fission, so that the fission rate remains constant and the energy is released steadily.
E.g. Nuclear reactor
Nuclear reactor + parts
Device in which self-sustaining controlled reaction is produced in a fissionable material.
- Fuel
- Moderator
- Control rods
- Coolant
- Shield
- Safety device
Fuel- nuclear reactor
Fissionable material
E.g. 92U235, Pu239 (Plutonium)
Control rods
- Rods of cadmium or boron which are used to control the fission rate in the reactor
- Cadmium and boron are good absorbers of slow neutrons
- So when rods are pushed into the reactor, fission rate decreases and when they are pulled out, fission rate increases
Coolant
Energy released inside the reactor in the form of heat is removed by coolant
E.g. air, water, CO2
Shield
To protect people working near the reactor from injurious radiations, thick concrete walls are erected outside the reactor
Safety device
In the case of an accident or an emergency, a special set of control rods, known as shut off rods enter the reactor automatically. Absorb the neutrons immediately.
Critical size and mass
Minimum size of fissioning material for sustained fission reaction to develop
if r > 1/K — process starts
if r < 1/K — process stops
Utilisation of energy output of nuclear reactor
- Production of Neutron Beam: The fast moving neutrons emitted by fission of U235 are converged into a fine beam for artificial disintegration of other elements
- Production of artificial radio-isotopes:
- Generation of energy: Energy is used to produce steam which operates a turbine and turns an electrical generator
Nuclear fusion
Process in which two light nuclei moving at high speeds fuse together to form a single nucleus
The mass of product nucleus is less than the masses of the individual nuclei which were fused
The lost mass is converted into energy which is released in the process
Conditions for nuclear fusion to take place
- Temperature: Of the order 108 K
- High kinetic energies (≅0.1 MeV)
- It is called a thermonuclear reaction because such high temperatures are required
- distance bw nuclei: 1.2 fm = 1.2 x 10-15 m
Stellar energy and thermonuclear energy
Energy obtained continuously from the stars by nuclear fusion
T/F
energy in fusion < energy in fission
false
Proton cycle rxn
fusion of two protons into deuterium
41H1 —> 2He4 + 21β0 + 2𝛎 + 2γ