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The binding energy of deuteron is 2.2 Me...

The binding energy of deuteron is 2.2 MeV and that of H`""_(2)^(4)He` is 28MeV. If two deuterons are fused to form one `""_(2)^(4)He` then the energy released is:-

A

25.8 MeV

B

23.6 MeV

C

19.2 MeV

D

30.2 MeV

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To find the energy released when two deuterons are fused to form one helium atom, we will use the binding energy values given in the problem. ### Step-by-Step Solution: 1. **Identify the Binding Energies:** - The binding energy of a deuteron (D) is given as \( B_D = 2.2 \, \text{MeV} \). - The binding energy of helium-4 (\( ^4He \)) is given as \( B_{He} = 28 \, \text{MeV} \). 2. **Write the Fusion Reaction:** - The fusion of two deuterons can be represented as: \[ 2D \rightarrow ^4He + \text{Energy} \] 3. **Calculate the Total Binding Energy of the Reactants:** - Since we have two deuterons, the total binding energy for the reactants is: \[ \text{Total Binding Energy of Reactants} = 2 \times B_D = 2 \times 2.2 \, \text{MeV} = 4.4 \, \text{MeV} \] 4. **Calculate the Binding Energy of the Product:** - The binding energy of the product (helium-4) is: \[ \text{Binding Energy of Product} = B_{He} = 28 \, \text{MeV} \] 5. **Calculate the Energy Released:** - The energy released during the fusion process can be calculated using the formula: \[ \text{Energy Released} = \text{Binding Energy of Product} - \text{Total Binding Energy of Reactants} \] - Substituting the values: \[ \text{Energy Released} = 28 \, \text{MeV} - 4.4 \, \text{MeV} = 23.6 \, \text{MeV} \] 6. **Final Answer:** - The energy released when two deuterons are fused to form one helium atom is \( \boxed{23.6 \, \text{MeV}} \).

To find the energy released when two deuterons are fused to form one helium atom, we will use the binding energy values given in the problem. ### Step-by-Step Solution: 1. **Identify the Binding Energies:** - The binding energy of a deuteron (D) is given as \( B_D = 2.2 \, \text{MeV} \). - The binding energy of helium-4 (\( ^4He \)) is given as \( B_{He} = 28 \, \text{MeV} \). ...
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