The displacement of the particle is given by:
\[ x = \frac{2R}{\frac{2mv}{qB}} \] where \( R \) is the radius of the circular path, \( m \) is the mass of the particle, \( v \) is its velocity, \( q \) is its charge, and \( B \) is the magnetic field strength.
Substituting \( v = \frac{2qV}{m} \), we get:
\[ x = \frac{2 \cdot m \cdot \frac{2qV}{m}}{qB} \] Simplifying: \[ x = \frac{4m(qV)}{qB} \] For a proton (\( H^+ \)): \[ x = 4 \, \text{cm} \]
The displacement is proportional to the square root of the mass: \[ x \propto \sqrt{m} \] Thus, for \( \text{AM} = 144 \) (144 times the proton mass): \[ x = 4 \, \text{cm} \cdot \sqrt{144} = 4 \cdot 12 = 48 \, \text{cm} \]
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