363692 Statement A :
The binding energy per nucleon, for nuclei with atomic mass number \(A\) > 100, decrease with \(A\).
Statement B :
Repulsive forces among nuclei are more for heavier nuclei.

363693 Read the Assertion and Reason carefully to mark the correct options given below:
Assertion :
The binding energy per nucleon is practically independent of the atomic number for nuclei of mass number in the range 30 to 170
Reason :
Nuclear force is short ranged.

363694 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 \(MeV\) while that of fragmentsis 8.5 \(MeV\). The total gain in the Binding Energy in the process is

363695 The binding energy of deutron \(_1^2{\text{H}}\) is \(1.112\,MeV\) per nucleon and an \(\alpha \)-particle \({}_2^4He\) has a binding energy of \(7.047\,MeV\) per nucleon. Then in the fusion reaction \(_1^2{\text{H}} + _1^2{\text{H}} \to _2^4{\text{He}} + Q,\) the energy \(Q\) released is

363696 Binding energy per nucleon \(vs\) mass number curve for nuclei is shown. \(W, X, Y\) and \(Z\) are four nuclei indicated on the curve. The process that would release energy is

363692 Statement A :
The binding energy per nucleon, for nuclei with atomic mass number \(A\) > 100, decrease with \(A\).
Statement B :
Repulsive forces among nuclei are more for heavier nuclei.

363693 Read the Assertion and Reason carefully to mark the correct options given below:
Assertion :
The binding energy per nucleon is practically independent of the atomic number for nuclei of mass number in the range 30 to 170
Reason :
Nuclear force is short ranged.

363694 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 \(MeV\) while that of fragmentsis 8.5 \(MeV\). The total gain in the Binding Energy in the process is

363695 The binding energy of deutron \(_1^2{\text{H}}\) is \(1.112\,MeV\) per nucleon and an \(\alpha \)-particle \({}_2^4He\) has a binding energy of \(7.047\,MeV\) per nucleon. Then in the fusion reaction \(_1^2{\text{H}} + _1^2{\text{H}} \to _2^4{\text{He}} + Q,\) the energy \(Q\) released is

363696 Binding energy per nucleon \(vs\) mass number curve for nuclei is shown. \(W, X, Y\) and \(Z\) are four nuclei indicated on the curve. The process that would release energy is

363692 Statement A :
The binding energy per nucleon, for nuclei with atomic mass number \(A\) > 100, decrease with \(A\).
Statement B :
Repulsive forces among nuclei are more for heavier nuclei.

363693 Read the Assertion and Reason carefully to mark the correct options given below:
Assertion :
The binding energy per nucleon is practically independent of the atomic number for nuclei of mass number in the range 30 to 170
Reason :
Nuclear force is short ranged.

363694 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 \(MeV\) while that of fragmentsis 8.5 \(MeV\). The total gain in the Binding Energy in the process is

363695 The binding energy of deutron \(_1^2{\text{H}}\) is \(1.112\,MeV\) per nucleon and an \(\alpha \)-particle \({}_2^4He\) has a binding energy of \(7.047\,MeV\) per nucleon. Then in the fusion reaction \(_1^2{\text{H}} + _1^2{\text{H}} \to _2^4{\text{He}} + Q,\) the energy \(Q\) released is

363696 Binding energy per nucleon \(vs\) mass number curve for nuclei is shown. \(W, X, Y\) and \(Z\) are four nuclei indicated on the curve. The process that would release energy is

363692 Statement A :
The binding energy per nucleon, for nuclei with atomic mass number \(A\) > 100, decrease with \(A\).
Statement B :
Repulsive forces among nuclei are more for heavier nuclei.

363693 Read the Assertion and Reason carefully to mark the correct options given below:
Assertion :
The binding energy per nucleon is practically independent of the atomic number for nuclei of mass number in the range 30 to 170
Reason :
Nuclear force is short ranged.

363694 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 \(MeV\) while that of fragmentsis 8.5 \(MeV\). The total gain in the Binding Energy in the process is

363695 The binding energy of deutron \(_1^2{\text{H}}\) is \(1.112\,MeV\) per nucleon and an \(\alpha \)-particle \({}_2^4He\) has a binding energy of \(7.047\,MeV\) per nucleon. Then in the fusion reaction \(_1^2{\text{H}} + _1^2{\text{H}} \to _2^4{\text{He}} + Q,\) the energy \(Q\) released is

363696 Binding energy per nucleon \(vs\) mass number curve for nuclei is shown. \(W, X, Y\) and \(Z\) are four nuclei indicated on the curve. The process that would release energy is

363692 Statement A :
The binding energy per nucleon, for nuclei with atomic mass number \(A\) > 100, decrease with \(A\).
Statement B :
Repulsive forces among nuclei are more for heavier nuclei.

363693 Read the Assertion and Reason carefully to mark the correct options given below:
Assertion :
The binding energy per nucleon is practically independent of the atomic number for nuclei of mass number in the range 30 to 170
Reason :
Nuclear force is short ranged.

363694 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 \(MeV\) while that of fragmentsis 8.5 \(MeV\). The total gain in the Binding Energy in the process is

363695 The binding energy of deutron \(_1^2{\text{H}}\) is \(1.112\,MeV\) per nucleon and an \(\alpha \)-particle \({}_2^4He\) has a binding energy of \(7.047\,MeV\) per nucleon. Then in the fusion reaction \(_1^2{\text{H}} + _1^2{\text{H}} \to _2^4{\text{He}} + Q,\) the energy \(Q\) released is

363696 Binding energy per nucleon \(vs\) mass number curve for nuclei is shown. \(W, X, Y\) and \(Z\) are four nuclei indicated on the curve. The process that would release energy is