363712 When a uranium isotope \({}_{92}^{235}U\) is bombarded witha neutron, ,it generates \({}_{36}^{89}Kr\), three neutrons and:

363713 In a fission process, nucleus \(A\) divides into two nuclei \(B\) and \(C\), their binding energies being \({E_a},{E_b}\) and \({E_c}\) respectively. Then

363714 Nuclear energy is released in fission since binding energy per nucleon is

363715 In a nuclear fission reaction of an isotope of mass \(M\). Three similar daughter nuclei of same mass are formed. The speed of a daughter nuclei in terms of mass defect \(\Delta M\) will be

363716 A nuclear explosive is designed to deliver \(1\,MW\) power in the form of heat energy. If the explosion is designed with nuclear fuel consisting of \(U^{235}\) to run a reactor at this power level for one year, then the amount of fuel needed is (take, energy per fission is \(200\,MeV\))

363712 When a uranium isotope \({}_{92}^{235}U\) is bombarded witha neutron, ,it generates \({}_{36}^{89}Kr\), three neutrons and:

363713 In a fission process, nucleus \(A\) divides into two nuclei \(B\) and \(C\), their binding energies being \({E_a},{E_b}\) and \({E_c}\) respectively. Then

363714 Nuclear energy is released in fission since binding energy per nucleon is

363715 In a nuclear fission reaction of an isotope of mass \(M\). Three similar daughter nuclei of same mass are formed. The speed of a daughter nuclei in terms of mass defect \(\Delta M\) will be

363716 A nuclear explosive is designed to deliver \(1\,MW\) power in the form of heat energy. If the explosion is designed with nuclear fuel consisting of \(U^{235}\) to run a reactor at this power level for one year, then the amount of fuel needed is (take, energy per fission is \(200\,MeV\))

363712 When a uranium isotope \({}_{92}^{235}U\) is bombarded witha neutron, ,it generates \({}_{36}^{89}Kr\), three neutrons and:

363713 In a fission process, nucleus \(A\) divides into two nuclei \(B\) and \(C\), their binding energies being \({E_a},{E_b}\) and \({E_c}\) respectively. Then

363714 Nuclear energy is released in fission since binding energy per nucleon is

363715 In a nuclear fission reaction of an isotope of mass \(M\). Three similar daughter nuclei of same mass are formed. The speed of a daughter nuclei in terms of mass defect \(\Delta M\) will be

363716 A nuclear explosive is designed to deliver \(1\,MW\) power in the form of heat energy. If the explosion is designed with nuclear fuel consisting of \(U^{235}\) to run a reactor at this power level for one year, then the amount of fuel needed is (take, energy per fission is \(200\,MeV\))

363712 When a uranium isotope \({}_{92}^{235}U\) is bombarded witha neutron, ,it generates \({}_{36}^{89}Kr\), three neutrons and:

363713 In a fission process, nucleus \(A\) divides into two nuclei \(B\) and \(C\), their binding energies being \({E_a},{E_b}\) and \({E_c}\) respectively. Then

363714 Nuclear energy is released in fission since binding energy per nucleon is

363715 In a nuclear fission reaction of an isotope of mass \(M\). Three similar daughter nuclei of same mass are formed. The speed of a daughter nuclei in terms of mass defect \(\Delta M\) will be

363716 A nuclear explosive is designed to deliver \(1\,MW\) power in the form of heat energy. If the explosion is designed with nuclear fuel consisting of \(U^{235}\) to run a reactor at this power level for one year, then the amount of fuel needed is (take, energy per fission is \(200\,MeV\))

363712 When a uranium isotope \({}_{92}^{235}U\) is bombarded witha neutron, ,it generates \({}_{36}^{89}Kr\), three neutrons and:

363713 In a fission process, nucleus \(A\) divides into two nuclei \(B\) and \(C\), their binding energies being \({E_a},{E_b}\) and \({E_c}\) respectively. Then

363714 Nuclear energy is released in fission since binding energy per nucleon is

363715 In a nuclear fission reaction of an isotope of mass \(M\). Three similar daughter nuclei of same mass are formed. The speed of a daughter nuclei in terms of mass defect \(\Delta M\) will be

363716 A nuclear explosive is designed to deliver \(1\,MW\) power in the form of heat energy. If the explosion is designed with nuclear fuel consisting of \(U^{235}\) to run a reactor at this power level for one year, then the amount of fuel needed is (take, energy per fission is \(200\,MeV\))