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Question: Paragraph for question nos. (16-17) Meson is composed of two sub-atomic particles and the interacti...

Paragraph for question nos. (16-17) Meson is composed of two sub-atomic particles and the interaction between the sub-atomic particles is complicated. Research of meson can be done by studying the collisions between the meson and high energy electron. As the collision is quite complicated, scientists invented a simplified model called "parton model" to grasp the main content during collision. In the model, the electron first collides with pan of meson (e.g. one of the sub-atomic particles) elastically. Then the energy and momentum are transferred to the other sub-atomic particles and thus the whole meson during subsequent interaction. This simplified model is described by the following: [figure] An electron of mass mm and energy E0E_0 collides with a neutral sub-atomic particles of mass m1m_1 in a meson. The other neutral sub-atomic particles in the meson has mass m2m_2. The sub-atomic particles are connected by a massless spring at natural length LL which is at equilibrium before collision. All movements are on a straight line and neglect the effect of relativity. Find, after collision. (given m1=5mm_1=5m & m2=2m1m_2=2m_1)

  1. The energy gain by the sub-atomic particle of mass m1m_1 due to collision is E0x\frac{E_0}{x}. Find xx

  2. The minimum kinetic energy of the meson as a whole system is E0y\frac{E_0}{y}. Find the value of yy.

A

x = 9/5

B

x = 5/9

C

y = 27/5

D

y = 5/27

Answer
  1. x=95x = \frac{9}{5}, 17. y=275y = \frac{27}{5}
Explanation

Solution

Question 16: The collision is elastic between the electron (mass mm, initial velocity vev_e) and particle m1m_1 (mass m1m_1, initially at rest). Initial energy of electron: E0=12mve2E_0 = \frac{1}{2} m v_e^2. Final velocity of m1m_1 after elastic collision: v1=2mm+m1vev_1' = \frac{2m}{m + m_1} v_e. Given m1=5mm_1 = 5m, so v1=2mm+5mve=2m6mve=13vev_1' = \frac{2m}{m + 5m} v_e = \frac{2m}{6m} v_e = \frac{1}{3} v_e. Energy gain by m1m_1: ΔKE1=12m1(v1)2=12(5m)(13ve)2=59(12mve2)=59E0\Delta KE_1 = \frac{1}{2} m_1 (v_1')^2 = \frac{1}{2} (5m) \left(\frac{1}{3} v_e\right)^2 = \frac{5}{9} \left(\frac{1}{2} m v_e^2\right) = \frac{5}{9} E_0. Given ΔKE1=E0x\Delta KE_1 = \frac{E_0}{x}, so 59E0=E0x    x=95\frac{5}{9} E_0 = \frac{E_0}{x} \implies x = \frac{9}{5}.

Question 17: The kinetic energy of the meson's center of mass (KECMKE_{CM}). KECM=12(m1+m2)VCM2KE_{CM} = \frac{1}{2} (m_1 + m_2) V_{CM}^2. Momentum of meson system after collision: Pmeson=m1v1P_{meson} = m_1 v_1'. VCM=Pmesonm1+m2=m1v1m1+m2V_{CM} = \frac{P_{meson}}{m_1 + m_2} = \frac{m_1 v_1'}{m_1 + m_2}. KECM=(m1v1)22(m1+m2)KE_{CM} = \frac{(m_1 v_1')^2}{2(m_1 + m_2)}. Given m1=5mm_1 = 5m and m2=2m1=10mm_2 = 2m_1 = 10m, so m1+m2=15mm_1 + m_2 = 15m. v1=13vev_1' = \frac{1}{3} v_e, and ve2=2E0mv_e^2 = \frac{2E_0}{m}. KECM=(5m)2(13ve)22(15m)=25m2192E0m30m=25m2E0930m=50270E0=527E0KE_{CM} = \frac{(5m)^2 \left(\frac{1}{3} v_e\right)^2}{2(15m)} = \frac{25m^2 \cdot \frac{1}{9} \frac{2E_0}{m}}{30m} = \frac{25m \cdot \frac{2E_0}{9}}{30m} = \frac{50}{270} E_0 = \frac{5}{27} E_0. Since VCMV_{CM} is constant, KECMKE_{CM} is the minimum kinetic energy. Given KECM=E0yKE_{CM} = \frac{E_0}{y}, so 527E0=E0y    y=275\frac{5}{27} E_0 = \frac{E_0}{y} \implies y = \frac{27}{5}.