363718 Consider the nuclear fission reaction \({{ }_{0}^{1} n+{ }_{92}^{235} U \rightarrow{ }_{56}^{144} B a+{ }_{36}^{89} K r+3{ }_{0}^{1} n}\). Assuming all the kinetic energy is carried away by the fast neutrons only and total binding energies of \({{ }_{92}^{235} {U},{ }_{56}^{144} {Ba}}\), and \({{ }_{36}^{89} {Kr}}\) to be \(1800\,MeV\), \(1200\,MeV\) and \(780\,MeV\) respectively, the average kinetic energy carried by each fast neutron is (in \(MeV\))
363719
In a fission reaction \(_{92}^{236}U{ \to ^{117}}X{ + ^{117}}Y + n + n,\) the average binding energy per nucleon of \(X\) and \(Y\) is \(8.5\,MeV\) whereas that of \({ }^{236} U\) is \(7.6\,MeV\).
The total energy liberated will be about :
\({ }_{92}^{236} U \rightarrow{ }^{117} X+{ }^{117} Y+n+n\)
363718 Consider the nuclear fission reaction \({{ }_{0}^{1} n+{ }_{92}^{235} U \rightarrow{ }_{56}^{144} B a+{ }_{36}^{89} K r+3{ }_{0}^{1} n}\). Assuming all the kinetic energy is carried away by the fast neutrons only and total binding energies of \({{ }_{92}^{235} {U},{ }_{56}^{144} {Ba}}\), and \({{ }_{36}^{89} {Kr}}\) to be \(1800\,MeV\), \(1200\,MeV\) and \(780\,MeV\) respectively, the average kinetic energy carried by each fast neutron is (in \(MeV\))
363719
In a fission reaction \(_{92}^{236}U{ \to ^{117}}X{ + ^{117}}Y + n + n,\) the average binding energy per nucleon of \(X\) and \(Y\) is \(8.5\,MeV\) whereas that of \({ }^{236} U\) is \(7.6\,MeV\).
The total energy liberated will be about :
\({ }_{92}^{236} U \rightarrow{ }^{117} X+{ }^{117} Y+n+n\)
363718 Consider the nuclear fission reaction \({{ }_{0}^{1} n+{ }_{92}^{235} U \rightarrow{ }_{56}^{144} B a+{ }_{36}^{89} K r+3{ }_{0}^{1} n}\). Assuming all the kinetic energy is carried away by the fast neutrons only and total binding energies of \({{ }_{92}^{235} {U},{ }_{56}^{144} {Ba}}\), and \({{ }_{36}^{89} {Kr}}\) to be \(1800\,MeV\), \(1200\,MeV\) and \(780\,MeV\) respectively, the average kinetic energy carried by each fast neutron is (in \(MeV\))
363719
In a fission reaction \(_{92}^{236}U{ \to ^{117}}X{ + ^{117}}Y + n + n,\) the average binding energy per nucleon of \(X\) and \(Y\) is \(8.5\,MeV\) whereas that of \({ }^{236} U\) is \(7.6\,MeV\).
The total energy liberated will be about :
\({ }_{92}^{236} U \rightarrow{ }^{117} X+{ }^{117} Y+n+n\)
363718 Consider the nuclear fission reaction \({{ }_{0}^{1} n+{ }_{92}^{235} U \rightarrow{ }_{56}^{144} B a+{ }_{36}^{89} K r+3{ }_{0}^{1} n}\). Assuming all the kinetic energy is carried away by the fast neutrons only and total binding energies of \({{ }_{92}^{235} {U},{ }_{56}^{144} {Ba}}\), and \({{ }_{36}^{89} {Kr}}\) to be \(1800\,MeV\), \(1200\,MeV\) and \(780\,MeV\) respectively, the average kinetic energy carried by each fast neutron is (in \(MeV\))
363719
In a fission reaction \(_{92}^{236}U{ \to ^{117}}X{ + ^{117}}Y + n + n,\) the average binding energy per nucleon of \(X\) and \(Y\) is \(8.5\,MeV\) whereas that of \({ }^{236} U\) is \(7.6\,MeV\).
The total energy liberated will be about :
\({ }_{92}^{236} U \rightarrow{ }^{117} X+{ }^{117} Y+n+n\)