Column I Column II A Nuclear fusion 1 E=mc2 B Nuclear fission 2 Generally possible for nuclei with low atomic number C β-decay 3 Generally possible for nuclei with higher atomic number D Mass-energy 4 Essentially proceeds by equivalence weak reaction nuclear forces

Question

Column I Column II A Nuclear fusion 1 E=mc2 B Nuclear fission 2 Generally possible for nuclei with low atomic number C β-decay 3 Generally possible for nuclei with higher atomic number D Mass-energy 4 Essentially proceeds by equivalence weak reaction nuclear forces (A)  (A) arrow(2) ; (B) arrow(3) ; (C) arrow(4); (D) arrow(1) (B) (A) arrow (4); (B) arrow(1); (C)arrow (2); (D) arrow (4) (C) (A) arrow (1); (B) arrow(3); (C) arrow (2); (D) arrow (4) (D) ( A ) arrow(3) ; (B) arrow(4) ;( C ) arrow(2) ;( D ) arrow(1)

Tardigrade Admin · Accepted Answer

(A) arrow(2) ;(B) arrow(3) ;(C) arrow(4) ;(D) arrow(1)

Q.

Column I Column II

A Nuclear fusion 1 $E = m c^{2}$

B Nuclear fission 2 Generally possible for nuclei with low atomic number

C $β$ -decay 3 Generally possible for nuclei with higher atomic number

D Mass-energy 4 Essentially proceeds by equivalence weak reaction nuclear forces

$(A) \to (2); (B) \to (3); (C) \to (4); (D) \to (1)$

$(A) \to (4); (B) \to (1); (C) \to (2); (D) \to (4)$

$(A) \to (1); (B) \to (3); (C) \to (2); (D) \to (4)$

$(A) \to (3); (B) \to (4); (C) \to (2); (D) \to (1)$

$(A) \to (2); (B) \to (3); (C) \to (4); (D) \to (1)$

Column I		Column II
A	Nuclear fusion	1	$E = m c^{2}$
B	Nuclear fission	2	Generally possible for nuclei with low atomic number
C	$β$ -decay	3	Generally possible for nuclei with higher atomic number
D	Mass-energy	4	Essentially proceeds by equivalence weak reaction nuclear forces

Q. Column I Column II A Nuclear fusion 1 E=mc2 B Nuclear fission 2 Generally possible for nuclei with low atomic number C β-decay 3 Generally possible for nuclei with higher atomic number D Mass-energy 4 Essentially proceeds by equivalence weak reaction nuclear forces

(A)→(2);(B)→(3);(C)→(4);(D)→(1)

(A)→(4);(B)→(1);(C)→(2);(D)→(4)

(A)→(1);(B)→(3);(C)→(2);(D)→(4)

(A)→(3);(B)→(4);(C)→(2);(D)→(1)

(A)→(2);(B)→(3);(C)→(4);(D)→(1)

Q.

Column I Column II

A Nuclear fusion 1 $E = m c^{2}$

B Nuclear fission 2 Generally possible for nuclei with low atomic number

C $β$ -decay 3 Generally possible for nuclei with higher atomic number

D Mass-energy 4 Essentially proceeds by equivalence weak reaction nuclear forces

$(A) \to (2); (B) \to (3); (C) \to (4); (D) \to (1)$

$(A) \to (4); (B) \to (1); (C) \to (2); (D) \to (4)$

$(A) \to (1); (B) \to (3); (C) \to (2); (D) \to (4)$

$(A) \to (3); (B) \to (4); (C) \to (2); (D) \to (1)$

$(A) \to (2); (B) \to (3); (C) \to (4); (D) \to (1)$