The energy gained by the electron when accelerated through a potential \(V\) is given by: \[ E = eV \] Where \(e\) is the charge of the electron and \(V\) is the potential. The kinetic energy of the electron when it strikes the anode is: \[ E = \frac{1}{2} m v^2 \] Equating the two expressions for energy: \[ eV = \frac{1}{2} m v^2 \] Solving for \(v\) (speed of the electron): \[ v = \sqrt{\frac{2eV}{m}} \] Substituting the values for the charge of the electron \(e = 1.6 \times 10^{-19} \, \text{C}\), the mass of the electron \(m = 9.1 \times 10^{-31} \, \text{kg}\), and \(V = 1200 \, \text{V}\): \[ v = \sqrt{\frac{2 \times (1.6 \times 10^{-19}) \times 1200}{9.1 \times 10^{-31}}} \] This simplifies to: \[ v \approx 2.1 \times 10^7 \, \text{ms}^{-1} \]
If \( \lambda \) and \( K \) are de Broglie wavelength and kinetic energy, respectively, of a particle with constant mass. The correct graphical representation for the particle will be:
One of the equations that are commonly used to define the wave properties of matter is the de Broglie equation. Basically, it describes the wave nature of the electron.
Very low mass particles moving at a speed less than that of light behave like a particle and waves. De Broglie derived an expression relating to the mass of such smaller particles and their wavelength.
Plank’s quantum theory relates the energy of an electromagnetic wave to its wavelength or frequency.
E = hν …….(1)
E = mc2……..(2)
As the smaller particle exhibits dual nature, and energy being the same, de Broglie equated both these relations for the particle moving with velocity ‘v’ as,
This equation relating the momentum of a particle with its wavelength is de Broglie equation and the wavelength calculated using this relation is the de Broglie wavelength.