Nuclear equations are vital for representing nuclear reactions occurring in stars and other cosmic events. They display how particles change during fusion reactions and maintain the conservation of mass and charge. In a nuclear equation, we reflect the atoms involved as well as their transformations.
When writing a nuclear equation, we must ensure both sides balance. This means that the total number of protons and neutrons (mass number) is consistent across the equation, just like the total charge (atomic number).
- The left side of the equation shows the reactants, or starting particles.
- The right side shows the products, or resulting particles after the reaction.
For example, when two protons, denoted as \( ^{1}_{1}\mathrm{H} \), combine, they form a deuterium \( ^{2}_{1}\mathrm{H} \) and a positron \( e^{+} \). The nuclear equation capturing this reaction looks like: \( ^{1}_{1}\mathrm{H} + ^{1}_{1}\mathrm{H} \rightarrow ^{2}_{1}\mathrm{H} + e^{+} \). This balance exemplifies how each element transforms in the star's heart.