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[" (c) From the relation "R=R(0)A^(1/3)"...

[" (c) From the relation "R=R_(0)A^(1/3)" ,where "R_(0)" is a constant and "A" is mass "],[" number of nucleus,show that the nuclear density is nearly constant."],[" (i.e.independent of "A)" ."]

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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)

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 = RoA^(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 (.e. Independent of A)

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