A circular trajectory occurs when the magnetic field is perpendicular to the velocity direction. Writing down the 2nd Newton's law for an arbitrary charged particle, we obtain:
"q v B = m a = \\frac{m v^2}{R}" Hence,
"R = \\frac{m v}{q B}"Kinetic energy of a particle is defined as follows:
"E_k=\\frac{m v^2}{2} = \\frac{(mv)^2}{2m} \\, \\Rightarrow \\, mv = \\sqrt{2m E_k}" As a result,
"R = \\frac{\\sqrt{2 E_k}}{B} \\frac{\\sqrt{m}}{q}" Hence, the ratio of radii is
"R_1 : R_2 : R_3 = \\frac{\\sqrt{m_1}}{q_1} : \\frac{\\sqrt{m_2}}{q_2} : \\frac{\\sqrt{m_3}}{q_3}" For a proton, a deuteron and alpha particle we have:
"proton: \\quad m_1 = m_0, \\, q_1 = q_0 \\\\\ndeuteron: \\quad m_2 = 2m_0, \\, q_2 = q_0\\\\\n\\alpha-particle: \\quad m_3 = 4m_0, \\, q_3 = 2q_0" Hence,
"R_1 : R_2 : R_3 = 1 : \\sqrt{2} : 1"
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