To solve the problem of finding the threshold wavelength for a given metal surface illuminated by light, we use the photoelectric effect equation. The photoelectric equation relates the kinetic energy of ejected electrons to the frequency of the incident light and the work function of the material:
\(E_k = h(f - f_0)\)
where:
The stopping potential \(V_s\) is related to the kinetic energy by:
\(E_k = eV_s\)
where \(e\) is the elementary charge.
We also have the relationship between frequency and wavelength:
\(f = \frac{c}{\lambda}\)
where \(c\) is the speed of light.
Substitute this into the photoelectric equation:
\(eV_s = h\frac{c}{\lambda} - h\frac{c}{\lambda_0}\)
For two different stopping potentials, we can write two equations:
Now, we solve these equations to find \(\lambda_0\), the threshold wavelength.
Rewrite Equation 1:
\(h \frac{c}{\lambda_0} = h \frac{c}{\lambda} - 8e\)
Rewrite Equation 2:
\(h \frac{c}{\lambda_0} = h \frac{c}{3\lambda} - 2e\)
Equating the two expressions for \(h \frac{c}{\lambda_0}\):
\(h \frac{c}{\lambda} - 8e = h \frac{c}{3\lambda} - 2e\)
Isolate terms:
\(h \frac{c}{\lambda} - h \frac{c}{3\lambda} = 8e - 2e\)
\(h c \left( \frac{1}{\lambda} - \frac{1}{3\lambda} \right) = 6e\)
Simplify:
\(h c \left( \frac{2}{3\lambda} \right) = 6e\)
\(h c = 9e \lambda\)
So, using Equation 1:
\(h \frac{c}{\lambda_0} = \frac{2}{3} \cdot 9e \lambda \Rightarrow \lambda_0 = 9\lambda\)
Thus, the threshold wavelength \(\lambda_0\) is 9\( \lambda \), and the correct answer is 9\( \lambda \).
\[ E = \phi + K_{\text{max}} \]
\[ \phi = \frac{hc}{\lambda_0} \]
\[ K_{\text{max}} = eV_0 \]
\[ 8e = \frac{hc}{\lambda} - \frac{hc}{\lambda_0} \quad \text{(i)} \]
\[ 2e = \frac{hc}{3\lambda} - \frac{hc}{\lambda_0} \quad \text{(ii)} \]
On solving (i) & (ii),
\[ \lambda_0 = 9\lambda \]

Nature of compounds TeO₂ and TeH₂ is___________ and ______________respectively.