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Consider one of fission reactions of ^(2...

Consider one of fission reactions of `^(235)U` by thermal neutrons `._(92)^(235)U +n rarr ._(38)^(94)Sr +._(54)^(140)Xe+2n` . The fission fragments are however unstable and they undergo successive `beta`-decay until `._(38)^(94)Sr` becomes `._(40)^(94)Zr` and `._(54)^(140)Xe` becomes `._(58)^(140)Ce`. The energy released in this process is
Given: `m(.^(235)U) =235.439u,m(n)=1.00866 u, m(.^(94)Zr)=93.9064 u, m(.^(140)Ce) =139.9055 u,1u=931 MeV]` .

A

`156 MeV`

B

`208 MeV`

C

`465 MeV`

D

cannot be computed

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The correct Answer is:
To solve the problem, we need to calculate the energy released during the fission of Uranium-235 by thermal neutrons, considering the masses of the reactants and products involved in the reaction. **Step 1: Identify the masses of the reactants.** The reactants in the fission reaction are: - Uranium-235: \( m(^{235}U) = 235.439 \, u \) - Neutron: \( m(n) = 1.00866 \, u \) So, the total mass of the reactants is: \[ m_{\text{reactants}} = m(^{235}U) + m(n) = 235.439 \, u + 1.00866 \, u = 236.44766 \, u \] **Step 2: Identify the masses of the products.** The products of the fission reaction after beta decay are: - Strontium-94: \( m(^{94}Sr) = 93.9064 \, u \) - Xenon-140: \( m(^{140}Xe) = 139.9055 \, u \) - 2 Neutrons: \( 2 \times m(n) = 2 \times 1.00866 \, u = 2.01732 \, u \) So, the total mass of the products is: \[ m_{\text{products}} = m(^{94}Sr) + m(^{140}Xe) + 2 \times m(n) = 93.9064 \, u + 139.9055 \, u + 2.01732 \, u = 235.82922 \, u \] **Step 3: Calculate the mass defect (\( \Delta m \)).** The mass defect is given by the difference between the mass of the reactants and the mass of the products: \[ \Delta m = m_{\text{reactants}} - m_{\text{products}} = 236.44766 \, u - 235.82922 \, u = 0.61844 \, u \] **Step 4: Convert the mass defect to energy (Q).** Using the conversion factor \( 1 \, u = 931 \, \text{MeV} \): \[ Q = \Delta m \times 931 \, \text{MeV} = 0.61844 \, u \times 931 \, \text{MeV/u} = 575.54 \, \text{MeV} \] **Final Answer:** The energy released in this fission reaction is approximately \( 575.54 \, \text{MeV} \). ---

To solve the problem, we need to calculate the energy released during the fission of Uranium-235 by thermal neutrons, considering the masses of the reactants and products involved in the reaction. **Step 1: Identify the masses of the reactants.** The reactants in the fission reaction are: - Uranium-235: \( m(^{235}U) = 235.439 \, u \) - Neutron: \( m(n) = 1.00866 \, u \) So, the total mass of the reactants is: ...
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Consider the case of bombardment of U^(235) nucleus with a thermal neutron. The fission products are Mo^(95) & La^(139) and two neutrons. Calculate the energy released by one U^(235) nucleus. (Rest masses of the nuclides are U^(235)=235.0439 u, ._(0)^(1)n=1.0087u, Mo^(95)=94.9058 u, La^(139).9061u) .

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Calculate the ground state Q value of the induced fission raction in the equation n+._(92)^(235) Urarr._(92)^(236)Uastrarr._(40)^(99)Zr+._(52)^(134)Te+2n If the neutron is thermal. A thermal neutorn is in thermal equilibrium with its envitronmnet, it has an avergae kinetic energy given by (3//2) kT . Given : m(n) =1.0087 am u, M(.^(235)U)=235.0439) am u , M(.^(99)Zr)=98.916 am u, M(.^(134)Te)=133.9115 am u .

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Consider two arbitaray decay equation and mark the correct alternative s given below. (i) ._(92)^(230)U rarr n+._(92)^(229)U (ii) ._(92_^(230)U rarr P +._(91)^(229)Pa Given: M(._(92)^(230)U) =230.033927 u,M(._(92)^(229)U)=229.03349 u, m_(n)=1.008665u , M(._(91)^(229)Pa) =229.032089, m_p =1.007825, 1 am u =931.5 MeV .

The number of neutrons accompanying the formation of ._(54)Xe^(139) and ._(38)Sr^(94) from the absorption of a slow neutron by ._(92)U^(235) , followed by nuclear fission is

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