Problem 181
Question
A stream of electrons from a heated filament was passed between two charged plates kept at a potential difference \(\mathrm{V}\) esu. If e and \(\mathrm{m}\) are charge and mass of an electron, respectively, then the value of \(\mathrm{h} / \lambda\) (where \(\lambda\) is wavelength associated with electron wave) is given by: \([2016]\) (a) \(2 \mathrm{meV}\) (b) \(\sqrt{\mathrm{meV}}\) (c) \(\sqrt{2 \mathrm{meV}}\) (d) meV
Step-by-Step Solution
Verified Answer
(c) \( \sqrt{2meV} \)
1Step 1: Understand the problem
We need to find the value of \( \frac{h}{\lambda} \) for electrons accelerated by a potential difference \( V \). We use the concepts of electron dynamics and De Broglie's wavelength.
2Step 2: Relation between velocity and potential difference
When an electron is accelerated by a potential difference \( V \), its kinetic energy \( KE \) is equal to \( eV \), where \( e \) is the charge of the electron. Also, \( KE = \frac{1}{2}mv^2 \), where \( m \) is the mass and \( v \) is the velocity of the electron. Equating both, we get \( \frac{1}{2}mv^2 = eV \), leading to \( v = \sqrt{\frac{2eV}{m}} \).
3Step 3: Apply De Broglie's hypothesis
De Broglie's wavelength \( \lambda \) is given by \( \lambda = \frac{h}{p} \), where \( p \) is the linear momentum. The linear momentum \( p \) can be expressed as \( mv \). Plug in the velocity from Step 2 to get \( p = m \cdot \sqrt{\frac{2eV}{m}} \) simplifying to \( \sqrt{2meV} \).
4Step 4: Calculate the value of \( \frac{h}{\lambda} \)
From \( \lambda = \frac{h}{p} \) and \( p = \sqrt{2meV} \), we calculate \( \frac{h}{\lambda} = p = \sqrt{2meV} \).
5Step 5: Verify against options
The derived expression \( \sqrt{2meV} \) matches option (c).
Key Concepts
De Broglie WavelengthKinetic EnergyPotential DifferenceElectron Velocity
De Broglie Wavelength
De Broglie wavelength is a fundamental concept in quantum mechanics that describes the wave-like nature of particles. According to Louis de Broglie's hypothesis, all matter exhibits wave-like properties, and the wavelength associated with a particle is known as its De Broglie wavelength. It is expressed by the equation: \[ \lambda = \frac{h}{p} \] where
- \( \lambda \) is the De Broglie wavelength,
- \( h \) is Planck’s constant, and
- \( p \) is the momentum of the particle.
Kinetic Energy
Kinetic energy is the energy that a particle possesses due to its motion. For an electron, kinetic energy can be calculated based on its velocity. The formula for kinetic energy \( KE \) is: \[ KE = \frac{1}{2}mv^2 \] where
- \( m \) is the mass of the electron, and
- \( v \) is its velocity.
Potential Difference
A potential difference, often measured in volts, refers to the difference in electric potential energy per unit charge between two points. For electrons, this concept is crucial as it describes how much energy is provided to or taken from the electron as it moves through an electric field. When an electron is accelerated by a potential difference \( V \), it gains kinetic energy stated by the equation: \[ KE = eV \] Here,
- \( e \) is the charge of the electron,
- \( V \) is the potential difference in volts.
Electron Velocity
Electron velocity is a key element in understanding electron dynamics as it affects both the kinetic energy and the momentum, thereby influencing the De Broglie wavelength. When an electron is subject to a potential difference \( V \), the velocity \( v \) of the electron can be approximated using the derived formula: \[ v = \sqrt{\frac{2eV}{m}} \] Here,
- \( e \) is the charge of the electron,
- \( V \) is the potential difference, and
- \( m \) is the mass.
Other exercises in this chapter
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