Step 1: Threshold Wavelength and Threshold Frequency Threshold Wavelength: Threshold wavelength \( \lambda_0 \) is the longest wavelength of incident light that can cause photoemission. It is related to the work function \( \phi \) of the material by the equation: \[ \lambda_0 = \frac{hc}{\phi} \] If the wavelength \( \lambda \) of the incident light is greater than \( \lambda_0 \), photoemission does not occur.
Threshold Frequency: Threshold frequency \( \nu_0 \) is the minimum frequency of the incident light required to eject electrons from the metal surface. It is given by: \[ \nu_0 = \frac{\phi}{h} \] If the frequency \( \nu \) of the incident light is less than \( \nu_0 \), no photoelectric emission occurs. \[ \boxed{\lambda_0 = \frac{hc}{\phi}, \quad \nu_0 = \frac{\phi}{h}} \] \
Step 2: Factors affecting Saturation Current and Cut-off Voltage Saturation Current: Saturation current is the maximum current obtained when all photoelectrons emitted from the surface reach the anode.
It depends on: - Intensity of Incident Light: As the intensity increases, more photons strike the surface, resulting in the emission of more electrons. \[ \text{Saturation current} \propto \text{Intensity of light} \]
Cut-off Voltage: Cut-off voltage (stopping potential) is the minimum negative potential required to stop the photoelectrons from reaching the anode.
It depends on: - Frequency of Incident Light: Higher frequency photons carry more energy, requiring a higher cut-off voltage to stop the electrons. Using Einstein's photoelectric equation: \[ eV_{\text{cut-off}} = h\nu - \phi \] \[ \boxed{\text{Saturation current} \propto \text{intensity}, \quad V_{\text{cut-off}} \propto \text{frequency.}} \]
Find the values of \( x, y, z \) if the matrix \( A \) satisfies the equation \( A^T A = I \), where
\[ A = \begin{bmatrix} 0 & 2y & z \\ x & y & -z \\ x & -y & z \end{bmatrix} \]
(b) Order of the differential equation: $ 5x^3 \frac{d^3y}{dx^3} - 3\left(\frac{dy}{dx}\right)^2 + \left(\frac{d^2y}{dx^2}\right)^4 + y = 0 $