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Column-I
Column - II
(A) Nuclear fusion
(1) \( \mathrm{E}=m \mathrm{c}^{2} \)
(B) Nuclear fission
(2) Generally possible for nuclei with low atomic number
(C) \( \beta \)-decay
(3) Generally possible for nuclei with higher atomic number
(D) Mass-energy
(4) Essentially proceeds by equivalence weak reaction nuclear forces
(a) (A) \( \rightarrow \) (2); (B) \( \rightarrow \) (3); (C) \( \rightarrow \) (4); (D) \( \rightarrow \) (1)
(b) (A) \( \rightarrow \) (4); (B) \( \rightarrow \) (1); (C) \( \rightarrow \) (2); (D) \( \rightarrow \) (4)
(c) (A) \( \rightarrow \) (1); (B) \( \rightarrow \) (3); (C) \( \rightarrow \) (2); (D) \( \rightarrow \) (4)
\( \mathrm{P} \)
(d) \( \quad \) (A) \( \rightarrow \) (3); (B) \( \rightarrow \) (4); (C) \( \rightarrow \) (2); (D) \( \rightarrow \) (1)
W
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