A. 1200
B. 900
C. 300
D. 1400
D
Ta có:
\(\begin{array}{l}
\overrightarrow {{p_p}} = \overrightarrow {{p_{\alpha 1}}} + \overrightarrow {{p_{\alpha 2}}} \Rightarrow {m_p}{v_p} = 2{m_\alpha }{v_\alpha }\cos \left( {\frac{\beta }{2}} \right)\\
\Rightarrow \cos \left( {\frac{\beta }{2}} \right) = \frac{1}{2}\left( {\frac{{{m_p}}}{{{m_\alpha }}}} \right)\left( {\frac{{{v_p}}}{{{v_\alpha }}}} \right)(1)\\
\Delta E = 2{K_\alpha } - {K_p} > 0 \Rightarrow 2\left( {\frac{1}{2}{m_\alpha }v_\alpha ^2} \right) > \frac{1}{2}{m_p}v_p^2 \Rightarrow \frac{{{v_p}}}{{{v_\alpha }}} < \sqrt {\frac{{2{m_\alpha }}}{{{m_p}}}} (2)\\
(1),(2) \Rightarrow \cos \left( {\frac{\beta }{2}} \right) < \frac{1}{2}\left( {\frac{{{m_p}}}{{{m_\alpha }}}} \right)\sqrt {\frac{{2{m_\alpha }}}{{{m_p}}}} = \frac{1}{2}\left( {\frac{1}{4}} \right)\sqrt {\frac{{2.\left( 4 \right)}}{1}} \approx 0,35 \Rightarrow \beta > {139^0}
\end{array}\)
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