91Ó°ÊÓ

In this exercise, understanding the concept of kinetic energy is crucial to analyze the movement of electrons. When electrons are accelerated through a potential difference, they gain kinetic energy. This energy can be expressed as a function of the charge of the electron and the potential difference applied, represented by the equation:\[ KE = eV \]where:

• \( KE \) is the kinetic energy
• \( e \) is the elementary charge, approximately \( 1.6 \times 10^{-19} \, \text{C} \)
• \( V \) is the potential difference

The kinetic energy gained allows us to find the velocity of the electrons using the expression:\[ KE = \frac{1}{2}mv^2 \]Rearranging gives the velocity:\[ v = \sqrt{\frac{2eV}{m}} \]Here, \( m \) is the mass of an electron, approximately \( 9.11 \times 10^{-31} \, \text{kg} \). Calculating kinetic energy is fundamental for determining the electron speed and examining if relativistic effects are significant.

The de Broglie wavelength is a key concept in quantum mechanics linking momentum to wave-like properties of particles. According to de Broglie's hypothesis, particles such as electrons exhibit wave-like characteristics, described by their wavelength:\[ \lambda = \frac{h}{mv} \]where:

• \( \lambda \) is the de Broglie wavelength
• \( h \) is Planck's constant, \( 6.626 \times 10^{-34} \, \text{Js} \)
• \( m \) is the mass of the electron
• \( v \) is the speed of the electron obtained previously

Understanding the de Broglie wavelength is essential in calculating diffraction patterns, like in this exercise where electrons pass through a slit. Their wavelengths contribute to the interference patterns observed, much like light waves, but on a quantum scale. The computed wavelength helps determine the positions of diffraction minima when electrons interact with the slit.

Assessing whether to use relativistic mechanics is crucial in electron beam problems. Electrons, when accelerated to high speeds, may need relativistic equations if their velocity nears a significant fraction of light speed. This scenario occurs when an electron's speed is a considerable portion of the speed of light, approximately:\[ 0.1c \]Here, \( c \) is the speed of light, \( 3 \times 10^8 \, \text{m/s} \). In this specific exercise, if the calculated velocity surpasses this threshold, relativistic adjustments are necessary. This would involve using the relativistic kinetic energy formula:\[ KE = (\gamma - 1)mc^2 \]with \( \gamma \) being the Lorentz factor:\[ \gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}} \]However, if the electron speed is much less than \( 0.1c \), classical mechanics provides sufficient accuracy for all computations.

The concept of diffraction minimum is central to understanding how electrons create a diffraction pattern after passing through a slit. When waves, including particle waves like electrons, pass through slits, they exhibit behavior characterized by constructive and destructive interference. For a diffraction minimum, where no or minimal wave intensity is observed, the condition is given by the formula:\[ a \sin \theta = n\lambda \]where:

• \( a \) is the slit width
• \( \theta \) is the angle at which minimum occurs
• \( n \) is the order of the minimum, with 1 being the first minimum
• \( \lambda \) is the wavelength of electrons as per de Broglie's relation

To find the slit width, the wavelength calculated before is used along with the observed angle \( \theta = 14.6^\circ \), leading to solving for \( a \). Knowing diffraction minima aids in measuring slit dimensions and understanding wave-particle duality in quantum mechanics.