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Zorluk: Çok zorNatural Radioactivity and Radiation Emissions

An α\alpha-particle (charge +2e+2e, mass mαm_\alpha) and a β\beta^--particle (charge e-e, mass mβm_\beta) emitted during natural radioactive decay enter a region containing uniform, mutually perpendicular electric (EE) and magnetic (BB) fields. Both particles move along paths perpendicular to both fields and traverse the region without undergoing any deflection. What is the ratio of the kinetic energy of the α\alpha-particle to that of the β\beta^--particle, Ek,αEk,β\frac{E_{k,\alpha}}{E_{k,\beta}}?

  1. mαmβ\frac{m_\alpha}{m_\beta}Cevap
  2. B
    11
  3. C
    22
  4. D
    mα2mβ\frac{m_\alpha}{2m_\beta}

Cevap

The ratio of their kinetic energies is equal to the ratio of their masses, mαmβ\frac{m_\alpha}{m_\beta}.
In crossed uniform electric and magnetic fields acting as a velocity selector, a charged particle passes undeflected when the electric force qEqE balances the magnetic Lorentz force qvBqvB. Equating these forces yields v=EBv = \frac{E}{B}, which depends only on field strengths and is independent of mass and charge. Because both the α\alpha-particle and β\beta^--particle traverse undeflected, both possess the same speed vv. Substituting equal speeds into the kinetic energy formula Ek=12mv2E_k = \frac{1}{2}mv^2 leaves the ratio of their kinetic energies equal to the ratio of their rest masses, mαmβ\frac{m_\alpha}{m_\beta}.

Adım Adım Çözüm

1
Apply the force balance condition for particles moving undeflected in crossed electric and magnetic fields.
Electric force magnitude FE=qEF_E = qE must equal magnetic force magnitude FB=qvBF_B = qvB, giving qE=qvB    v=EBqE = qvB \implies v = \frac{E}{B}.
For zero net deflection, the electrostatic force and magnetic Lorentz force must be equal in magnitude and opposite in direction.
2
Determine the velocities of the α\alpha-particle and β\beta^--particle.
vα=EBv_\alpha = \frac{E}{B} and vβ=EBv_\beta = \frac{E}{B}, so vα=vβ=vv_\alpha = v_\beta = v.
The velocity selection equation v=EBv = \frac{E}{B} is completely independent of particle mass mm and charge qq.
3
Express the ratio of the kinetic energies of the two emissions using Ek=12mv2E_k = \frac{1}{2}mv^2.
Ek,αEk,β=12mαv212mβv2=mαmβ\frac{E_{k,\alpha}}{E_{k,\beta}} = \frac{\frac{1}{2} m_\alpha v^2}{\frac{1}{2} m_\beta v^2} = \frac{m_\alpha}{m_\beta}.
Since the speed vv is identical for both particles, the 12v2\frac{1}{2}v^2 terms cancel out completely.

Anahtar Kavram

Velocity selector behavior and kinetic energy dependence of radiation emissions in electromagnetic fields
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