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Nuclei Test - 63

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Nuclei Test - 63
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  • Question 1
    1 / -0
    Binding energy per nucleon vs. mass number curve for nuclei is shown in fig. W, X, Y and Z are four nuclei indicated on the curve. The process that would release energy is

    Solution
    Binding energy of $$W$$,  $$|E_W| = 120\times7.5=900$$  MeV
    Binding energy of $$Y$$,  $$|E_Y| = 30\times8.5=255$$  MeV
    In process :  $$W\rightarrow 2Y$$
    $$Q$$ value,  $$Q = |E_W| - |E_Y| = 900-2(255) =390$$  MeV
    As $$Q$$ value is positive, thus energy is released in process   $$W\rightarrow 2Y$$
  • Question 2
    1 / -0
    Biding energy is equal to: (m is the mass defect in amu)
    Solution
    From mass energy equivalence Binding energy,
    $$E=\triangle m{ c }^{ 2 }\\ \because { c }^{ 2 }=931MeV\\ E=\triangle m \times 931MeV$$
  • Question 3
    1 / -0
    The binding energies per nucleon for a deuteron and an  -particle are  $${ x }_{ 1} ,{ x}_{ 2 }$$ respectively. What will be the energy Q released in the reaction $$_{ 1 }^{ }{ { H }_{ }^{ 2 } }+_{ 1 }^{ }{ { H }_{ }^{ 2 } }\rightarrow _{ 2 }^{ }{ { He }_{ }^{ 4 } }+Q$$
    Solution

  • Question 4
    1 / -0
    The rest energy of an electron is $$0.511 MeV.$$ The electron is accelerated from rest to a velocity $$0.5 c$$. The change in its energy will be
    Solution
    $$\displaystyle mc^2=\dfrac{m_0}{\sqrt{1-\dfrac{v^2}{c^2}}}c^2=\frac{m_0}{\sqrt{1-\dfrac{(0.5c)^2}{c^2}}}c^2$$$$\displaystyle =\frac{m_0}{\sqrt{1-0.25}}c^2=\frac{m_0}{\sqrt{0.75}}c^2=1.15m_0c^2$$

    Change in energy $$= 1.15\:m_0c^2- m_0c^2$$
                                   $$=0.15\times 9.1 \times 10^{-31}\times(3\times  10^8)^2$$
                                   
    $$=12.285\times 10^{-15}J $$
                                   $$\displaystyle =\frac{12.285\times10^{-15}}{1.6\times10^{-13} }MeV$$
                                   $$= 0.07678\,MeV $$
  • Question 5
    1 / -0
    Results of calculations for four different designs of a fusion reactor using D-D reaction are given below. Which of these is most promising based on Lawson criterion?
    Solution
    According to Lawson, deuteron density (n) and confinement tome $$t_0$$ must satisfy the criterion
    $$nt_0 > 5\times 10^{14} cm^{-3}s$$
    This condition is satisfied only by choice(b) for which $$nt_0=(8.0\times 10^{14})\times (9.0\times 10^{-1})=7.2\times 10^{14}cm^{-3}s$$. Hence the correct choice is $$(b)$$.

  • Question 6
    1 / -0
    Assume that two deutron nuclei in the core of fusion reactor at temperature $$T$$ are moving towards each other,each with kinetic energy $$1.5kT$$, when the separation between them is large enough to neglect Coulomb potential energy. Also neglect any interaction from other particles in the core. The minimum temperature $$T$$ required for them to reach a separation of $$4\times { 10 }^{ -15 }$$m is in the range
    Solution
    Applying conservation of mechanical energy, we get:
    Loss of kinetic energy of two deuteron nuclei $$=$$ Gain in their potential energy.
    $$\Rightarrow 2\times 1.5kT=\displaystyle\frac { 1 }{ 4\pi \varepsilon _{ 0 } } \frac { e\times e }{ r } $$
    $$\Rightarrow 2\times 1.5\left( 8.6\times { 10 }^{ -5 }\frac { eV }{ K }  \right) \times T=\displaystyle \frac { \left( 1.44\times { 10 }^{ -9 }eVm \right)  }{ 4\times { 10 }^{ -15 }m } $$
    $$\Rightarrow T=\displaystyle \frac { 1.44\times { 10 }^{ -9 } }{ 2\times 1.5\times 8.6\times { 10 }^{ -15 }\times 4\times { 10 }^{ -15 } } $$$$=0.0139\times { 10 }^{ 11 }=1.4\times { 10 }^{ 9 }K$$
  • Question 7
    1 / -0

    Directions For Questions

    Some of the heavy nuclei decay into lighter nuclei by emitting a-particle and acquire stability. The principles of conservation of atomic number, mass number, linear momentum and energy (including rest mass energy) are valid for these decays.
    A stationary nucleus $$^{226}_{88}Ra$$ (ground state) decays into the nucleus $$^{222}_{86}Rn$$ (ground state) by emitting an $$\alpha - particle$$.
    Given that $$m(^{226}_{88}Ra)=226.02540 u$$. $$m(^4_2He)=4.00260 u$$. $$m(^{222}_{86}Rn)=222.01750 u$$.

    ...view full instructions

    The Q-value for the $$\alpha-decay$$ of $$^{226}_{88}Ra$$ is (approximately)
    Solution
    $$ \begin{array}{c} _{88}^{226} Ra \longrightarrow{ }_{2}^{4} He^{2+}+{ }_{86}^{222} Rn \end{array} $$ 
    $$ 226.02540 \mu \quad 4.00260 \mu \quad 222.01750 \mu $$ 
    $$ \begin{aligned} \Delta m=& 0.0053 \\ Q \text { -value } &=\Delta m \times 931.5 \mathrm{MeV} \\ &=0.0053 \times 931.5 \\ &=4.93695 \end{aligned} $$
  • Question 8
    1 / -0
    Which of the following nuclear reactions is not possible?
    Solution
    The following laws hold true in any reaction
    1) Conservation of mass (nucleons)
    2) conservation of charge
    Checking for all the reactions
    $$\Sigma A_{products} = \Sigma A_{reactants}$$
    For option C: $$ 9 +4 \ne 11+1$$
    Hence, option (c) not possible.
  • Question 9
    1 / -0
    The velocity of a body of rest mass $$m_o$$ is $$\dfrac{\sqrt 3}{2} c$$ (where c is the velocity of light in vacuum). The mass of this body is : 
    Solution
    By special theory of relativity
    $$m' = \gamma m= \cfrac{m_0}{\sqrt{1 -\cfrac{v^2}{c^2}}}$$
    $$m' = \cfrac{m_0}{\sqrt{1 -\cfrac{3}{4}}} =\cfrac{m_0}{(1/2)}= 2m_0$$
  • Question 10
    1 / -0
    Calculate the binding energy of $$_{3}^{6}\textrm{Li}$$ assuming the mass of $$_{3}^{6}\textrm{Li}$$ atom as $$6.01512$$ amu:
    Solution
    Mass defect is
    $$\Delta m = [Zm_p + (A - Z)m_n-M]$$
    $$m_p =$$ mass of the proton $$= 1.007277 amu$$
    $$m_n =$$ mass of the neutron $$= 1.008655 amu$$
    Mass of the bound $$_{3}^{6}\textrm{Li}$$, lithium has three protons and three neutrons, since $$Z = 3, A = 6$$ and number of neutrons $$=A -Z=6-3=3)$$

    $$\therefore \Delta m = [3 \times 1.007277 + 3(1.008655] - 6.01512$$
                                       $$=[3.02183 + 3.02596] - 6.01512$$
                                       $$= 6.047795 - 6.01512 = 0.032675 amu.$$
    But the energy equivalent of $$1 amu = 931 MeV$$
    Therefore, the binding energy which is equal to the energy equivalent of mass defect in amu is
    $$E_b =\Delta m \times 931 MeV$$
    $$= 0.032675 \times 931 = 30.42 MeV$$
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