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WorksheetsHSSTV 2
Total questions: 83
Worksheet time: 7hrs 55mins
The radius of a nucleus is given by
R=R0A
R=R0A1/3
R=R0A2/3
R=R0A
The approximate value of the nuclear radius constant R0 is
0.01 fm
1.2 fm
10 fm
100 fm
The density of nuclear matter is
Different for different nuclei
Much less than atomic density
Nearly constant for all nuclei
Proportional to atomic number
The constancy of nuclear density implies that
R∝A
R∝A1/3
M∝A2/3
Nuclear force is long range
Most stable nuclei in ground state are approximately
Cubical in shape
Cylindrical in shape
Spherical in shape
Irregular in shape
Non-spherical shape of heavy nuclei is mainly due to
Gravitational attraction
Coulomb repulsion
Weak interaction
Pairing force
In the liquid drop model, nucleus is compared to a drop of liquid because
It has colour
It shows surface tension and incompressibility
It flows
It evaporates easily
The volume energy term in the semi-empirical mass formula is due to
Coulomb repulsion
Surface nucleons
Short range nuclear force
Spin–orbit interaction
Surface energy term arises because
Protons repel each other
Neutrons are unstable
Surface nucleons have fewer neighbours
Nucleus rotates
Coulomb energy term in liquid drop model depends mainly on
Neutron number
Proton number
Mass defect
Nuclear spin
Symmetry energy term becomes important when
N=Z
N=Z
Z=0
A=1
Pairing energy is maximum when the nucleus has
Odd Z and odd N
Even Z and odd N
Odd Z and even N
Even Z and even N
Liquid drop model successfully explains
Magic numbers
Discrete energy levels
Nuclear fission
Spin–orbit splitting
Shell model of nucleus is analogous to
Planetary model
Liquid model
Atomic shell model
Solid state band model
Magic numbers in nuclei are explained by
Liquid drop model
Shell model
Bohr model
Classical mechanics
The origin of magic numbers is mainly due to
Coulomb force
Surface tension
Spin–orbit coupling
Gravitational force
A nucleus with both proton number and neutron number equal to magic numbers is
Highly unstable
Highly radioactive
Particularly stable
Highly deformed
The first magic number is
1
2
4
6
Binding energy of a nucleus is the energy required to
Remove one electron
Break nucleus into protons only
Break nucleus into its nucleons
Excite nucleus to higher state
Mass defect arises because
Some mass is lost as heat
Protons are heavier in nucleus
Part of mass converts into binding energy
Neutrons decay inside nucleus
The binding energy per nucleon is maximum for nuclei around
Hydrogen
Uranium
Iron
Deuterium
High binding energy per nucleon indicates that the nucleus is
Highly unstable
Weakly bound
Highly stable
Radioactive
The energy released in nuclear fission is mainly due to
Increase in mass
Decrease in mass (mass defect)
Chemical reaction
Change in atomic number only
According to the liquid drop model, nuclear force is
Long range
Repulsive only
Short range and attractive
Gravitational
In the semi-empirical mass formula, the term that accounts for proton–proton repulsion is
Volume term
Surface term
Coulomb term
Pairing term
The shell model assumes that nucleons move
Freely like gas molecules
In fixed orbits like electrons in atoms
As a rigid body
Only on the surface
Which of the following is a magic number?
10
14
20
26
The stability of doubly magic nuclei is explained by
Liquid drop model
Shell model
Bohr model
Classical mechanics
Spin–orbit coupling in nucleus results in
Nuclear fission
Splitting of energy levels
Pair production
Beta decay
The term in binding energy formula that reduces binding for large Z is
Volume term
Surface term
Coulomb term
Pairing term
Nuclear radius is independent of
Mass number
Nuclear density
Nuclear charge
Nuclear constant R0
The shape of a nucleus with closed shells is generally
Highly deformed
Elliptical
Spherical
Irregular
The pairing energy is zero for nuclei with
Even Z, even N
Odd Z, odd N
Even Z, odd N
Odd Z, even N
The liquid drop model fails to explain
Nuclear fission
Binding energy
Magic numbers
Nuclear density
The shell model explains nuclear stability in terms of
Surface tension
Coulomb repulsion
Closed energy shells
Gravitational force
The approximate radius of a nucleus with mass number 27 is
R0
3R0
9R0
27R0
A large binding energy per nucleon implies
Easy fission
Easy fusion
Greater stability
Radioactivity
The symmetry energy term favours
Large difference between N and Z
Equal number of protons and neutrons
In heavy nuclei, deviation from spherical shape is mainly due to
Nuclear force
Weak force
Coulomb repulsion
Pairing force
The shell model is particularly successful in explaining
Nuclear fission
Magic numbers and spin
Nuclear density
Surface tension
The binding energy of a nucleus is equal to
Δmc2
mc2
21mv2
hν
The unit commonly used for nuclear binding energy is
eV
keV
MeV
GeV
For light nuclei, energy is released mainly through
Fission
Fusion
Radioactivity
Ionisation
The liquid drop model predicts that the nucleus is
Compressible like gas
Incompressible like liquid
Elastic like solid
Rigid like crystal
Which term in the mass formula accounts for neutron–proton pairing?
Volume term
Surface term
Coulomb term
Pairing term
The most stable nuclei are those with
Very high Z
Very low A
Maximum binding energy per nucleon
Minimum binding energy
Magic numbers of neutrons or protons are
1, 3, 5, 7
2, 8, 20, 28, 50, 82, 126
4, 9, 16, 25
All even numbers
A doubly magic nucleus has
Equal N and Z
Both N and Z even
Both N and Z magic numbers
Very large mass number
Spin–orbit interaction in nucleus is
Very weak
Negligible
Responsible for magic numbers
Due to Coulomb force
The shell model treats nucleons as moving in
A common potential well
Free space
Circular orbits only
Surface layer only
The radius of a nucleus is proportional to
A
A1/2
A1/3
A2/3
The nearly constant nuclear density implies that
Nuclear force is long range
Nucleus is compressible
Volume is proportional to mass number
Surface area is proportional to mass number
The deformation of a nucleus is maximum for
Magic nuclei
Light nuclei
Heavy nuclei
Hydrogen
The surface energy term in liquid drop model decreases binding because
Surface nucleons are loosely bound
Protons repel each other
Neutrons decay
Spin–orbit coupling
Which model explains nuclear fission most successfully?
Shell model
Liquid drop model
Atomic model
Quantum field model
The shell model is a
Classical model
Semi-classical model
Quantum mechanical model
Relativistic model
The term responsible for stability of even–even nuclei is
Symmetry energy
Coulomb energy
Pairing energy
Volume energy
The binding energy curve shows that
Very heavy nuclei are most stable
Very light nuclei are most stable
Medium mass nuclei are most stable
All nuclei have same stability
Nuclear force between nucleons is
Long range and repulsive
Short range and attractive
Long range and attractive
Short range and repulsive only
The shell model cannot explain properly
Magic numbers
Nuclear spin
Nuclear fission
Nuclear magnetic moment
The binding energy per nucleon is lowest for
Iron
Carbon
Uranium
Helium
The mass of a nucleus is always
Equal to sum of masses of nucleons
Greater than sum of masses of nucleons
Less than sum of masses of nucleons
Independent of nucleons
The semi-empirical mass formula is based mainly on
Shell model
Liquid drop model
Atomic model
Quantum field theory
The symmetry energy term is minimum when
N=Z
N>Z
N<Z
Z=0
The pairing energy is positive for
Odd–odd nuclei
Even–even nuclei
Even–odd nuclei
Odd–even nuclei
The liquid drop model fails to explain
Nuclear fission
Nuclear density
Magic numbers
Binding energy trend
The shell model explains nuclear spin mainly due to
Orbital motion of nucleons
Surface vibration
Coulomb repulsion
Nuclear rotation only
A closed shell nucleus has
Minimum binding energy
Maximum deformation
Extra stability
High radioactivity
The nuclear radius increases with mass number because
Density decreases
Volume is proportional to A
Charge increases
Force weakens
The strong nuclear force is saturated because
It is long-range
Each nucleon interacts with all others
Each nucleon interacts only with nearest neighbours
It is repulsive
The most stable isotope of iron is around
A=12
A=28
A=56
A=238
The volume term in binding energy is proportional to
A
A2
A1/3
A2/3
The Coulomb term in mass formula is proportional to
Z
Z2
A
N
Which nucleus is expected to be most spherical?
Deformed heavy nucleus
Doubly magic nucleus
Odd-A nucleus
Very light nucleus
The shell model is most suitable for explaining
Nuclear fission
Nuclear fusion
Magic numbers
Surface tension
The pairing effect is absent in nuclei with
Even Z, even N
Odd Z, odd N
Even Z, odd N
Odd Z, even N
The deformation of a nucleus decreases when
Z increases
A increases
Shells are closed
Temperature increases
The binding energy per nucleon curve explains
Atomic spectra
Nuclear stability
Photoelectric effect
Compton effect
A large surface energy implies
Larger stability
Smaller binding
Larger mass defect
Larger radius only
The nucleus behaves like an incompressible fluid because
Nuclear force is weak
Nuclear force is long range
Nuclear density is constant
Nuclear mass is small
The binding energy per nucleon decreases for very heavy nuclei mainly due to
Surface energy
Symmetry energy
Coulomb repulsion
Pairing energy
The most stable nuclei are found near
A=1
A=20
A=56
A=238
The liquid drop model considers the nucleus to be
A collection of free particles
A rigid solid
An incompressible charged liquid drop
A gaseous system
