Новое решение
en/14.4.18.md
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| + | ### Statement | ||
| + | |||
| + | $14.4.18.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | Data: | ||
| + | |||
| + | Arc radius: $R = 0.3\ \text{m}$. | ||
| + | Magnetic flux density: $B = 1\ \text{T}$. | ||
| + | Elementary charge: $e = 1.6 \times 10^{-19}\ \text{C}$ | ||
| + | |||
| + | The kinetic energy of protons and electrons that pass through the magnet following this arc is requested. | ||
| + | |||
| + | Momentum–magnetic field relation | ||
| + | |||
| + | A particle of charge e moving perpendicular to a uniform magnetic field B describes a circular arc. The magnetic force $ F = e v B $ acts as the centripetal force. In relativity, the relation is: | ||
| + | |||
| + | $p = e B R$ | ||
| + | |||
| + | where p is the linear momentum | ||
| + | |||
| + | We calculate the momentum : | ||
| + | |||
| + | $p = (1.6 \times 10^{-19}\ \text{C}) \times (1\ \text{T}) \times (0.3\ \text{m}) = 4.8 \times 10^{-20}\ \text{kg·m/s}$ | ||
| + | |||
| + | To work with energies in MeV, we use pc | ||
| + | |||
| + | $pc = p \times c = 4.8 \times 10^{-20} \times 3 \times 10^8\ \text{m/s} | ||
| + | = 1.44 \times 10^{-11}\ \text{J}$ | ||
| + | |||
| + | Convert to $ MeV (1\ \text{MeV} = 1.6 \times 10^{-13}\ \text{J})$: | ||
| + | |||
| + | $pc = \frac{1.44 \times 10^{-11}}{1.6 \times 10^{-13}}\ \text{MeV} \approx 90\ \text{MeV}$. | ||
| + | |||
| + | Kinetic energy | ||
| + | |||
| + | The total energy E and momentum p are related to the rest mass $ m_0 c^2$: | ||
| + | |||
| + | $E^2 = (pc)^2 + (m_0 c^2)^2, \qquad K = E - m_0 c^2$. | ||
| + | |||
| + | We apply this to each particle. | ||
| + | |||
| + | Proton $(m_p c^2 \approx 938\ \text{MeV})$: | ||
| + | |||
| + | $K_p = \sqrt{90^2 + 938^2} - 938 | ||
| + | = \sqrt{8100 + 879844} - 938 | ||
| + | \approx \sqrt{887944} - 938 | ||
| + | \approx 942.3 - 938 | ||
| + | \approx 4.3\ \text{MeV}$ | ||
| + | |||
| + | The non‑relativistic approximation could also be used $(pc \ll m_p c^2)$: | ||
| + | |||
| + | $K_p \approx \frac{p^2}{2m_p} = \frac{(pc)^2}{2m_p c^2} = \frac{90^2}{2 \times 938} \approx 4.3\ \text{MeV}$ | ||
| + | |||
| + | Electron $(m_e c^2 \approx 0.511\ \text{MeV})$ | ||
| + | |||
| + | $K_e = \sqrt{90^2 + 0.511^2} - 0.511 | ||
| + | \approx \sqrt{8100 + 0.261} - 0.511 | ||
| + | \approx 90.0015 - 0.511 | ||
| + | \approx 89.5\ \text{MeV}$ | ||
| + | |||
| + | The electron is ultra‑relativistic: | ||
| + | $K_e \approx pc - m_e c^2 \approx 90 - 0.5 \approx 89.5\ \text{MeV}$ | ||
| + | |||
| + | 3. Final result | ||
| + | |||
| + | $\boxed{K_p \approx 4.3\ \text{MeV}}, \qquad $ | ||
| + | |||
| + | $\boxed{K_e \approx 89.5\ \text{MeV}}$ | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
| @@ -0,0 +1,74 @@ | |||
| ### Statement | |||
| $14.4.18.$ [Insert the problem statement] | |||
| ### Solution | |||
| Data: | |||
| Arc radius: $R = 0.3\ \text{m}$. | |||
| Magnetic flux density: $B = 1\ \text{T}$. | |||
| Elementary charge: $e = 1.6 \times 10^{-19}\ \text{C}$ | |||
| The kinetic energy of protons and electrons that pass through the magnet following this arc is requested. | |||
| Momentum–magnetic field relation | |||
| A particle of charge e moving perpendicular to a uniform magnetic field B describes a circular arc. The magnetic force $ F = e v B $ acts as the centripetal force. In relativity, the relation is: | |||
| $p = e B R$ | |||
| where p is the linear momentum | |||
| We calculate the momentum : | |||
| $p = (1.6 \times 10^{-19}\ \text{C}) \times (1\ \text{T}) \times (0.3\ \text{m}) = 4.8 \times 10^{-20}\ \text{kg·m/s}$ | |||
| To work with energies in MeV, we use pc | |||
| $pc = p \times c = 4.8 \times 10^{-20} \times 3 \times 10^8\ \text{m/s} | |||
| = 1.44 \times 10^{-11}\ \text{J}$ | |||
| Convert to $ MeV (1\ \text{MeV} = 1.6 \times 10^{-13}\ \text{J})$: | |||
| $pc = \frac{1.44 \times 10^{-11}}{1.6 \times 10^{-13}}\ \text{MeV} \approx 90\ \text{MeV}$. | |||
| Kinetic energy | |||
| The total energy E and momentum p are related to the rest mass $ m_0 c^2$: | |||
| $E^2 = (pc)^2 + (m_0 c^2)^2, \qquad K = E - m_0 c^2$. | |||
| We apply this to each particle. | |||
| Proton $(m_p c^2 \approx 938\ \text{MeV})$: | |||
| $K_p = \sqrt{90^2 + 938^2} - 938 | |||
| = \sqrt{8100 + 879844} - 938 | |||
| \approx \sqrt{887944} - 938 | |||
| \approx 942.3 - 938 | |||
| \approx 4.3\ \text{MeV}$ | |||
| The non‑relativistic approximation could also be used $(pc \ll m_p c^2)$: | |||
| $K_p \approx \frac{p^2}{2m_p} = \frac{(pc)^2}{2m_p c^2} = \frac{90^2}{2 \times 938} \approx 4.3\ \text{MeV}$ | |||
| Electron $(m_e c^2 \approx 0.511\ \text{MeV})$ | |||
| $K_e = \sqrt{90^2 + 0.511^2} - 0.511 | |||
| \approx \sqrt{8100 + 0.261} - 0.511 | |||
| \approx 90.0015 - 0.511 | |||
| \approx 89.5\ \text{MeV}$ | |||
| The electron is ultra‑relativistic: | |||
| $K_e \approx pc - m_e c^2 \approx 90 - 0.5 \approx 89.5\ \text{MeV}$ | |||
| 3. Final result | |||
| $\boxed{K_p \approx 4.3\ \text{MeV}}, \qquad $ | |||
| $\boxed{K_e \approx 89.5\ \text{MeV}}$ | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||