In nuclear equations, we need to ensure that both the atomic number (Z) and the mass number (A) are conserved on both sides of the equation.
For $_{11}^{24}\text{Na} \longrightarrow {}_{-1}^{0}\beta + \square$
The atomic number must be conserved: 11 = -1 + Z
Therefore, Z = 12
The mass number must be conserved: 24 = 0 + A
Therefore, A = 24
The missing particle is $_{12}^{24}\text{Mg}$
For $_{78}^{170}\text{Pt} \longrightarrow {}_{2}^{4}\alpha + \square$
The atomic number must be conserved: 78 = 2 + Z
Therefore, Z = 76
The mass number must be conserved: 170 = 4 + A
Therefore, A = 166
The missing particle is $_{76}^{166}\text{Os}$
For $_{54}^{118}\text{Xe} \longrightarrow {}_{53}^{118}\text{I} + \square$
The atomic number must be conserved: 54 = 53 + Z
Therefore, Z = 1
The mass number must be conserved: 118 = 118 + A
Therefore, A = 0
The missing particle is $_{1}^{0}\text{e}^{+}$ (positron)
- \( \boxed{{}_{12}^{24} \text{Mg}} \)
- \( \boxed{{}_{76}^{166} \text{Os}} \)
- \( \boxed{{}_{1}^{0} \text{e}^{+}} \)