147513 The binding energy of deuteron $\left({ }_{1}^{2} \mathrm{H}\right)$ is $\mathbf{1 . 1 5}$
$\mathrm{MeV}$ per nucleon and an alpha particle $\left({ }_{2}^{4} \mathrm{H}\right)$ has a binding energy 7. $1 \mathrm{MeV}$ per nucleon. Then in the reaction
${ }_{1}^{2} \mathrm{H}+{ }_{1}^{2} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+\mathrm{Q}$
the energy released $Q$ is

147516 In the reaction ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+{ }_{0}^{1} \mathrm{n}$, if the binding energies of ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H}$ and ${ }_{2}^{4} \mathrm{He}$ are respectively $\mathrm{a}, \mathrm{b}$ and $\mathrm{c}$ (in $\mathrm{MeV}$ ), then the energy (in $\mathrm{MeV}$ ) released in this reaction is

147518 The mass of a ${ }_{3}^{7} \mathrm{Li}$ nucleus is $0.042 \mathrm{u}$ less than the sum of the masses of all its nucleons. The binding energy per nucleon of ${ }_{3}^{7} \mathrm{Li}$ nucleus is nearly

147520 The mass density of a nucleus varies with mass number $A$ as

147521 The radius of germanium (Ge) nuclei is measured to be twice the radius of ${ }_{4}^{9} \mathrm{Be}$. The number of nucleons in $\mathrm{Ge}$ are

147513 The binding energy of deuteron $\left({ }_{1}^{2} \mathrm{H}\right)$ is $\mathbf{1 . 1 5}$
$\mathrm{MeV}$ per nucleon and an alpha particle $\left({ }_{2}^{4} \mathrm{H}\right)$ has a binding energy 7. $1 \mathrm{MeV}$ per nucleon. Then in the reaction
${ }_{1}^{2} \mathrm{H}+{ }_{1}^{2} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+\mathrm{Q}$
the energy released $Q$ is

147516 In the reaction ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+{ }_{0}^{1} \mathrm{n}$, if the binding energies of ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H}$ and ${ }_{2}^{4} \mathrm{He}$ are respectively $\mathrm{a}, \mathrm{b}$ and $\mathrm{c}$ (in $\mathrm{MeV}$ ), then the energy (in $\mathrm{MeV}$ ) released in this reaction is

147518 The mass of a ${ }_{3}^{7} \mathrm{Li}$ nucleus is $0.042 \mathrm{u}$ less than the sum of the masses of all its nucleons. The binding energy per nucleon of ${ }_{3}^{7} \mathrm{Li}$ nucleus is nearly

147520 The mass density of a nucleus varies with mass number $A$ as

147521 The radius of germanium (Ge) nuclei is measured to be twice the radius of ${ }_{4}^{9} \mathrm{Be}$. The number of nucleons in $\mathrm{Ge}$ are

147513 The binding energy of deuteron $\left({ }_{1}^{2} \mathrm{H}\right)$ is $\mathbf{1 . 1 5}$
$\mathrm{MeV}$ per nucleon and an alpha particle $\left({ }_{2}^{4} \mathrm{H}\right)$ has a binding energy 7. $1 \mathrm{MeV}$ per nucleon. Then in the reaction
${ }_{1}^{2} \mathrm{H}+{ }_{1}^{2} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+\mathrm{Q}$
the energy released $Q$ is

147516 In the reaction ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+{ }_{0}^{1} \mathrm{n}$, if the binding energies of ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H}$ and ${ }_{2}^{4} \mathrm{He}$ are respectively $\mathrm{a}, \mathrm{b}$ and $\mathrm{c}$ (in $\mathrm{MeV}$ ), then the energy (in $\mathrm{MeV}$ ) released in this reaction is

147518 The mass of a ${ }_{3}^{7} \mathrm{Li}$ nucleus is $0.042 \mathrm{u}$ less than the sum of the masses of all its nucleons. The binding energy per nucleon of ${ }_{3}^{7} \mathrm{Li}$ nucleus is nearly

147520 The mass density of a nucleus varies with mass number $A$ as

147521 The radius of germanium (Ge) nuclei is measured to be twice the radius of ${ }_{4}^{9} \mathrm{Be}$. The number of nucleons in $\mathrm{Ge}$ are

147513 The binding energy of deuteron $\left({ }_{1}^{2} \mathrm{H}\right)$ is $\mathbf{1 . 1 5}$
$\mathrm{MeV}$ per nucleon and an alpha particle $\left({ }_{2}^{4} \mathrm{H}\right)$ has a binding energy 7. $1 \mathrm{MeV}$ per nucleon. Then in the reaction
${ }_{1}^{2} \mathrm{H}+{ }_{1}^{2} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+\mathrm{Q}$
the energy released $Q$ is

147516 In the reaction ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+{ }_{0}^{1} \mathrm{n}$, if the binding energies of ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H}$ and ${ }_{2}^{4} \mathrm{He}$ are respectively $\mathrm{a}, \mathrm{b}$ and $\mathrm{c}$ (in $\mathrm{MeV}$ ), then the energy (in $\mathrm{MeV}$ ) released in this reaction is

147518 The mass of a ${ }_{3}^{7} \mathrm{Li}$ nucleus is $0.042 \mathrm{u}$ less than the sum of the masses of all its nucleons. The binding energy per nucleon of ${ }_{3}^{7} \mathrm{Li}$ nucleus is nearly

147520 The mass density of a nucleus varies with mass number $A$ as

147521 The radius of germanium (Ge) nuclei is measured to be twice the radius of ${ }_{4}^{9} \mathrm{Be}$. The number of nucleons in $\mathrm{Ge}$ are

147513 The binding energy of deuteron $\left({ }_{1}^{2} \mathrm{H}\right)$ is $\mathbf{1 . 1 5}$
$\mathrm{MeV}$ per nucleon and an alpha particle $\left({ }_{2}^{4} \mathrm{H}\right)$ has a binding energy 7. $1 \mathrm{MeV}$ per nucleon. Then in the reaction
${ }_{1}^{2} \mathrm{H}+{ }_{1}^{2} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+\mathrm{Q}$
the energy released $Q$ is

147516 In the reaction ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H} \rightarrow{ }_{2}^{4} \mathrm{He}+{ }_{0}^{1} \mathrm{n}$, if the binding energies of ${ }_{1}^{2} \mathrm{H}+{ }_{1}^{3} \mathrm{H}$ and ${ }_{2}^{4} \mathrm{He}$ are respectively $\mathrm{a}, \mathrm{b}$ and $\mathrm{c}$ (in $\mathrm{MeV}$ ), then the energy (in $\mathrm{MeV}$ ) released in this reaction is

147518 The mass of a ${ }_{3}^{7} \mathrm{Li}$ nucleus is $0.042 \mathrm{u}$ less than the sum of the masses of all its nucleons. The binding energy per nucleon of ${ }_{3}^{7} \mathrm{Li}$ nucleus is nearly

147520 The mass density of a nucleus varies with mass number $A$ as

147521 The radius of germanium (Ge) nuclei is measured to be twice the radius of ${ }_{4}^{9} \mathrm{Be}$. The number of nucleons in $\mathrm{Ge}$ are