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Suppose that an alpha particle of 3.20 MeV approaches head-on a lead nucleus (Z = 82). Assuming that the lead nucleus remains at rest and the alpha pa
Question

Suppose that an alpha particle of 3.20 MeV approaches head-on a lead nucleus (Z = 82). Assuming that the lead nucleus remains at rest and the alpha particle momentarily comes to rest and reverses its direction at a distance much more than the radius of the lead nucleus, the distance of its closest approach is:

A.

59.2 fm

B.

36.9 fm

C.

73.8 fm

D.

24.6 fm

Correct option is C

To calculate the distance of closest approach r, we equate the initial kinetic energy of the alpha particle to the electrostatic potential energy at the point of closest approach:14πε0Z1Z2e2r=K.E.Where:Z1=2 (alpha particle),Z2=82 (lead nucleus),e=1.6×1019 C,K.E.=3.20 MeV=3.20×106×1.6×1019 J,14πε0=9×109 Nm2/C2\text{To calculate the \textbf{distance of closest approach} } r, \text{ we equate the initial kinetic energy of the alpha particle to the electrostatic potential energy at the point of closest approach:} \\\frac{1}{4\pi \varepsilon_0} \cdot \frac{Z_1 Z_2 e^2}{r} = K.E. \\\\\text{Where:} \\\quad Z_1 = 2 \ (\text{alpha particle}), \\\quad Z_2 = 82 \ (\text{lead nucleus}), \\\quad e = 1.6 \times 10^{-19}\ \text{C}, \\\quad K.E. = 3.20\ \text{MeV} = 3.20 \times 10^6 \times 1.6 \times 10^{-19}\ \text{J}, \\\quad \frac{1}{4\pi \varepsilon_0} = 9 \times 10^9\ \text{Nm}^2/\text{C}^2

r=14πε0Z1Z2e2K.E.r = \frac{1}{4 \pi \varepsilon_0} \cdot \frac{Z_1 Z_2 e^2}{K.E.}

r=9×109×2×82×(1.6×1019)23.20×106×1.6×1019r=9×109×2×82×2.56×10385.12×1013r=3.78×10265.12×1013=7.38×1014 mConvert to femtometers (fm):r=73.8 fmr = \frac{9 \times 10^9 \times 2 \times 82 \times (1.6 \times 10^{-19})^2}{3.20 \times 10^6 \times 1.6 \times 10^{-19}} \\r = \frac{9 \times 10^9 \times 2 \times 82 \times 2.56 \times 10^{-38}}{5.12 \times 10^{-13}} \\r = \frac{3.78 \times 10^{-26}}{5.12 \times 10^{-13}} = 7.38 \times 10^{-14}\, \text{m} \\\\\text{Convert to femtometers (fm):} \\r = 73.8\, \text{fm}​​​​

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