266290 Statement I : H. Geiger and E. Marsden directed a beam of \(\alpha\)-particles emitted from a \({ }_{23}^{214} \mathrm{Bi}\) radioactive source at the thin metal foil of gold. Statement II : The impact parameter is the perpendicular distance of the final velocity vector of the \(\alpha\)-particle from the centre of nucleus.
266290 Statement I : H. Geiger and E. Marsden directed a beam of \(\alpha\)-particles emitted from a \({ }_{23}^{214} \mathrm{Bi}\) radioactive source at the thin metal foil of gold. Statement II : The impact parameter is the perpendicular distance of the final velocity vector of the \(\alpha\)-particle from the centre of nucleus.
266290 Statement I : H. Geiger and E. Marsden directed a beam of \(\alpha\)-particles emitted from a \({ }_{23}^{214} \mathrm{Bi}\) radioactive source at the thin metal foil of gold. Statement II : The impact parameter is the perpendicular distance of the final velocity vector of the \(\alpha\)-particle from the centre of nucleus.
266290 Statement I : H. Geiger and E. Marsden directed a beam of \(\alpha\)-particles emitted from a \({ }_{23}^{214} \mathrm{Bi}\) radioactive source at the thin metal foil of gold. Statement II : The impact parameter is the perpendicular distance of the final velocity vector of the \(\alpha\)-particle from the centre of nucleus.
266290 Statement I : H. Geiger and E. Marsden directed a beam of \(\alpha\)-particles emitted from a \({ }_{23}^{214} \mathrm{Bi}\) radioactive source at the thin metal foil of gold. Statement II : The impact parameter is the perpendicular distance of the final velocity vector of the \(\alpha\)-particle from the centre of nucleus.