The collision will be inelastic if a part of kinetic energy is used to excite the atom i.e. `K_(i)ne K_(f)`
By momentum conservation
`mv=mv_(1)+mv_(2)`
`v=v_(1)+v_(2)`
`(1)/(2)mv^(2)=(1)/(2)mv_(1)^(2)+(1)/(2)mv_(2)^(2)+DeltaE`
`v^(2)=v_(1)^(2)+v_(2)^(2)+(2DeltaE)/(m)`
`(v_(1)+v_(2))^(2)=v_(1)^(2)+v_(2)^(2)+(2DeltaE)/(m)`
`2v_(1) v_(2)=(2DeltaE)/(m) implies v_(1) v_(2)=(DeltaE)/(m)`
`(v_(1)-v_(2))^(2)=(v_(1)+v_(2))^(2)-4v_(1)v_(2)=v^(2)-(4DeltaE)/(m)`
As `(v_(1)-v_(2))` must be real
`(v_(1)-v_(2))^(2) ge 0`
`v^(2)-4 (DeltaE)/(m) ge0`
`(1)/(2) mv^(2) ge 2DeltaE`
Minimum K.E. to excite electron
`DeltaE=13.6((1)/(1^(2))-(1)/(2^(2)))=10.2 eV`
`((1)/(2) mv^(2))_(min) ge 2xx10.2`
`((1)/(2) mv^(2))_(min) ge 20.4 eV`
Minimum K.E. of neutron =20.4 eV