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The overall hydrogen burning reaction in stars can be represented as the conversion of four protons...

The overall hydrogen burning reaction in stars can be represented as the conversion of four protons to one α particle. Part A Use the data for the mass of H−1 and He−4 to calculate the energy released by this process. ANSWER NEEDS TO BE IN J/Mol of reactant

Solutions

Expert Solution

The fusion reaction in stars is given as follows:

4_1^1{H}2^{He}+ {2}}_0^{ + 1}e411​H→24​He+20+1​e

Mass on the reactant side:

4times left[ {(1 times .1.67262. times .{10}^{ - 27}) + (0 times .1.67493 .times {10}^{ - 27}) + (1 times 9.10939 times {10}^{ - 31})} right]

= 6.69874.times {10^{ - 27}{kg}4×[(1×1.67262×10−27)+(0×1.67493×10−27)+(1×9.10939×10−31)]

                   =6.69874×10−27kg

convert kg into joule by multiplying the value of 1000.

                  = 6.69874×10−24 j/mol    

Mass on the product side:

(2 times .1.67262 times {10^{ - 27}) + (2 times.1.67493times {10^{ - 27}) + (4times 9.10939 times {10^{ - 31}) = 6.69412 times {10^{ - 27}{kg}}(2×1.67262×10−27)+(2×1.67493×10−27)+(4×9.10939×10−31)

          =6.69412×10−27kg

convert kg into joule by multiplying the value of 1000.

          =6.69412×10−24 j/mol

There are 4 moles of 1^1{H}11​H atoms on the reactant side. One 1^1{H}1^1​Hatom contains 1 proton and 1 electron. Hence, the net mass on the reactant side is calculated as above. On the product side, 1 mole of 2^4{He}2^4​He atoms is produced and 2 moles of positron are produced. Hence, the net mass is calculated as above.

Nuclear reactions involve atomic nuclei undergoing changes. The difference of a nuclear reaction with respect to a chemical reaction is that usually there is transfer of subatomic particles, in the place of electrons, among the reactants (or emission from a single reactant), thus giving the products.

A broad classification of the nuclear reactions gives the following types:

Nuclear fission: It involves the splitting of a heavy nucleus into lighter nuclei. This is mostly initiated by bombardment of the nucleus with subatomic particles such as neutrons or lighter nuclei like the

{alpha }{ - }{{particle}}α−particle.


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