Step 1: Understanding the Concept (Photoelectric Effect):
This problem uses Einstein's photoelectric equation, which describes the energy balance when a photon strikes a metal surface and ejects an electron (a photoelectron). The energy of the incident photon is used partly to overcome the work function of the metal and the rest is converted into the kinetic energy of the ejected electron.
Step 2: Key Formula or Approach:
Einstein's photoelectric equation is:
\[ K.E._{max} = E_{photon} - \phi_0 \]
where:
\begin{itemize}
\item \(K.E._{max}\) is the maximum kinetic energy of the ejected photoelectron.
\item \(E_{photon}\) is the energy of the incident photon.
\item \(\phi_0\) is the work function of the metal.
\end{itemize}
The energy of a photon can be calculated from its wavelength \(\lambda\). A very useful shortcut for calculations where wavelength is in Angstroms (Å) and energy is needed in electron-volts (eV) is:
\[ E_{photon} (\text{in eV}) = \frac{hc}{e\lambda} \approx \frac{12400}{\lambda (\text{in Å})} \]
Step 3: Detailed Calculation:
\begin{enumerate}
\item Given Data:
\begin{itemize}
\item Wavelength of incident light, \(\lambda = 3300\) Å.
\item Work function of Cesium, \(\phi_0 = 1.9\) eV.
\end{itemize}
\item Calculate Photon Energy (\(E_{photon}\)):
Using the shortcut formula:
\[ E_{photon} = \frac{12400}{\lambda (\text{in Å})} \, \text{eV} = \frac{12400}{3300} \, \text{eV} \]
\[ E_{photon} = \frac{124}{33} \, \text{eV} \approx 3.757 \, \text{eV} \]
Let's use \(E_{photon} \approx 3.76\) eV for our calculation.
\item Calculate Maximum Kinetic Energy (\(K.E._{max}\)):
Now, substitute the values into the photoelectric equation:
\[ K.E._{max} = E_{photon} - \phi_0 \]
\[ K.E._{max} = 3.76 \, \text{eV} - 1.9 \, \text{eV} \]
\[ K.E._{max} = 1.86 \, \text{eV} \]
\end{enumerate}
Step 4: Final Answer:
The maximum kinetic energy of the ejected photo-electrons is 1.86 eV.
Given below are two statements: one is labelled as Assertion (A) and the other one is labelled as Reason (R).
Assertion (A): Emission of electrons in the photoelectric effect can be suppressed by applying a sufficiently negative electron potential to the photoemissive substance.
Reason (R): A negative electric potential, which stops the emission of electrons from the surface of a photoemissive substance, varies linearly with the frequency of incident radiation.
In light of the above statements, choose the most appropriate answer from the options given below: