147442 The mass of proton, neutron and helium nucleus are respectively $1.0073 \mathrm{u}, 1.0087 \mathrm{u}$ and $4.0015 \mathrm{u}$. The binding energy of helium nucleus is:

147446 The ratio of the density of oxygen nucleus $\left({ }_{8}^{16} \mathrm{O}\right)$ and helium nucleus $\left({ }_{2}^{4} \mathrm{He}\right)$ is

147447 Binding energy of a Nitrogen nucleus $\left[{ }_{7}^{14} \mathrm{~N}\right]$, given $\mathbf{m}\left[{ }_{7}^{14} \mathbf{N}\right]=\mathbf{1 4 . 0 0 3 0 7} \mathbf{u}$

147448 The ratio of the radii of the nuclei ${ }_{29} \mathrm{X}^{64}$ and ${ }_{84} \mathrm{X}^{216}$ is

147450 A nucleus with mass number 240 breaks into two fragments each of mass number 120, the binding energy per nucleon of unfragmented nuclei is 7.6 $\mathrm{MeV}$ while that of fragments is 8.5 $\mathrm{MeV}$.
The total gain in the binding energy in the process is

147442 The mass of proton, neutron and helium nucleus are respectively $1.0073 \mathrm{u}, 1.0087 \mathrm{u}$ and $4.0015 \mathrm{u}$. The binding energy of helium nucleus is:

147446 The ratio of the density of oxygen nucleus $\left({ }_{8}^{16} \mathrm{O}\right)$ and helium nucleus $\left({ }_{2}^{4} \mathrm{He}\right)$ is

147447 Binding energy of a Nitrogen nucleus $\left[{ }_{7}^{14} \mathrm{~N}\right]$, given $\mathbf{m}\left[{ }_{7}^{14} \mathbf{N}\right]=\mathbf{1 4 . 0 0 3 0 7} \mathbf{u}$

147448 The ratio of the radii of the nuclei ${ }_{29} \mathrm{X}^{64}$ and ${ }_{84} \mathrm{X}^{216}$ is

147450 A nucleus with mass number 240 breaks into two fragments each of mass number 120, the binding energy per nucleon of unfragmented nuclei is 7.6 $\mathrm{MeV}$ while that of fragments is 8.5 $\mathrm{MeV}$.
The total gain in the binding energy in the process is

147442 The mass of proton, neutron and helium nucleus are respectively $1.0073 \mathrm{u}, 1.0087 \mathrm{u}$ and $4.0015 \mathrm{u}$. The binding energy of helium nucleus is:

147446 The ratio of the density of oxygen nucleus $\left({ }_{8}^{16} \mathrm{O}\right)$ and helium nucleus $\left({ }_{2}^{4} \mathrm{He}\right)$ is

147447 Binding energy of a Nitrogen nucleus $\left[{ }_{7}^{14} \mathrm{~N}\right]$, given $\mathbf{m}\left[{ }_{7}^{14} \mathbf{N}\right]=\mathbf{1 4 . 0 0 3 0 7} \mathbf{u}$

147448 The ratio of the radii of the nuclei ${ }_{29} \mathrm{X}^{64}$ and ${ }_{84} \mathrm{X}^{216}$ is

147450 A nucleus with mass number 240 breaks into two fragments each of mass number 120, the binding energy per nucleon of unfragmented nuclei is 7.6 $\mathrm{MeV}$ while that of fragments is 8.5 $\mathrm{MeV}$.
The total gain in the binding energy in the process is

147442 The mass of proton, neutron and helium nucleus are respectively $1.0073 \mathrm{u}, 1.0087 \mathrm{u}$ and $4.0015 \mathrm{u}$. The binding energy of helium nucleus is:

147446 The ratio of the density of oxygen nucleus $\left({ }_{8}^{16} \mathrm{O}\right)$ and helium nucleus $\left({ }_{2}^{4} \mathrm{He}\right)$ is

147447 Binding energy of a Nitrogen nucleus $\left[{ }_{7}^{14} \mathrm{~N}\right]$, given $\mathbf{m}\left[{ }_{7}^{14} \mathbf{N}\right]=\mathbf{1 4 . 0 0 3 0 7} \mathbf{u}$

147448 The ratio of the radii of the nuclei ${ }_{29} \mathrm{X}^{64}$ and ${ }_{84} \mathrm{X}^{216}$ is

147450 A nucleus with mass number 240 breaks into two fragments each of mass number 120, the binding energy per nucleon of unfragmented nuclei is 7.6 $\mathrm{MeV}$ while that of fragments is 8.5 $\mathrm{MeV}$.
The total gain in the binding energy in the process is

147442 The mass of proton, neutron and helium nucleus are respectively $1.0073 \mathrm{u}, 1.0087 \mathrm{u}$ and $4.0015 \mathrm{u}$. The binding energy of helium nucleus is:

147446 The ratio of the density of oxygen nucleus $\left({ }_{8}^{16} \mathrm{O}\right)$ and helium nucleus $\left({ }_{2}^{4} \mathrm{He}\right)$ is

147447 Binding energy of a Nitrogen nucleus $\left[{ }_{7}^{14} \mathrm{~N}\right]$, given $\mathbf{m}\left[{ }_{7}^{14} \mathbf{N}\right]=\mathbf{1 4 . 0 0 3 0 7} \mathbf{u}$

147448 The ratio of the radii of the nuclei ${ }_{29} \mathrm{X}^{64}$ and ${ }_{84} \mathrm{X}^{216}$ is

147450 A nucleus with mass number 240 breaks into two fragments each of mass number 120, the binding energy per nucleon of unfragmented nuclei is 7.6 $\mathrm{MeV}$ while that of fragments is 8.5 $\mathrm{MeV}$.
The total gain in the binding energy in the process is