[" (7) "R=R_(0)A^(1/3)(R_(0)=" Constant,"A=mass" no.) "R=" snadius of "],[" muclews Taking the relation show that the nuclean "],[" density does not depend on mass mumber "A" ."]

R = R_0A^(1//3) ( R_0 = constant, A = Mass Number), R = radius of nucleus. Taking the relation show that of nuclear density does not depend on mass number A .

The radius of nucleus: R=R_0A^(1/3) ( R_0 =constant, A=mass No.). Taking the relation, show that the nuclear density does not depend on mass number A.

from the relation R=R_0A^(1//3) , where R_0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e., independent of A ).

form the relation R=R_0A^(1//3) , where R_0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e., independent of A ).

From the relation R=R_(0)A^(1//3) , where 'R_(0)' is a constant and 'A' is the mass number of a nucleus, show that the nuclear matter density is nearly constant.

From the relation R = R_0A^(1//3) , where R_0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

From the relation R = R_0A^(1/3) , where R_0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

From the relation R=R_0A^(1/3) , where R_0 is a constant and A is the mass number of a nucleus , show that the nuclear matter density is nearly constant.(i.e., independent of A)

R=R_(0)A^(1//3) , where R_(0) has the value: