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From the relation R=R(0)A^(1//3) where R...

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 (i.e. independent of A).

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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 ).

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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: