The alpha particle is emitted at 4235 m/s
Explanation:
We can use the law of conservation of momentum to solve the problem: the total momentum of the original nucleus must be equal to the total momentum after the alpha particle has been emitted. Therefore:
[tex]p_i = p_f\\ Mu=m_1 v_1 + m_2 v_2 =[/tex]
where:
[tex]M =222u [/tex] is the mass of the original nucleus
[tex]v=420 m/s[/tex] is the initial velocity of the nucleus
[tex]m_1 = 4 u[/tex] is the mass of the alpha particle
[tex]v_1[/tex] is the final velocity of the alpha particle
[tex]m_2 = 222u-4u = 218 u[/tex] is the mass of the daughter nucleus
[tex]v_2 = 350 m/s[/tex] is the final velocity of the nucleus
Solving for [tex]v_1[/tex], we find the final velocity of the alpha particle:
[tex]v_1 = \frac{Mu-m_2 v_2}{m_1}=\frac{(222)(420)-(218)(350)}{4}=4235 m/s[/tex]
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