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In a photoelectric emission, electrons a...

In a photoelectric emission, electrons are ejected from metals X and Y by light of frequency f. The potential difference V required to stop the electrons is measured for various frequencies.. If Y has a greater work function than X, which graph illustrates the expected results?

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To solve the problem regarding the photoelectric emission from metals X and Y, we need to analyze the relationship between the stopping potential (V) and the frequency (f) of the incident light. Here are the steps to arrive at the solution: ### Step 1: Understand the Work Function The work function (φ) of a metal is the minimum energy required to eject an electron from the surface of that metal. It is related to the threshold frequency (ν₀) by the equation: \[ \phi = h \nu_0 \] where \( h \) is Planck's constant. Given that metal Y has a greater work function than metal X, we can express this as: \[ \phi_Y > \phi_X \] This implies: \[ h \nu_{0Y} > h \nu_{0X} \] Thus, the threshold frequency for metal Y is greater than that for metal X: \[ \nu_{0Y} > \nu_{0X} \] ### Step 2: Einstein's Photoelectric Equation The stopping potential (V) is related to the frequency of the incident light (f) by Einstein's photoelectric equation: \[ eV = hf - \phi \] where \( e \) is the charge of the electron. For metals X and Y, we can write: 1. For metal X: \[ eV_X = hf - h\nu_{0X} \] Rearranging gives: \[ V_X = \frac{hf}{e} - \frac{h\nu_{0X}}{e} \] 2. For metal Y: \[ eV_Y = hf - h\nu_{0Y} \] Rearranging gives: \[ V_Y = \frac{hf}{e} - \frac{h\nu_{0Y}}{e} \] ### Step 3: Analyze the Graphs From the equations derived, we can see that both \( V_X \) and \( V_Y \) are linear functions of frequency \( f \) with the same slope of \( \frac{h}{e} \). However, the y-intercepts will differ due to the different work functions (or threshold frequencies). - The y-intercept for metal X will be at \( -\frac{h\nu_{0X}}{e} \). - The y-intercept for metal Y will be at \( -\frac{h\nu_{0Y}}{e} \). Since \( \nu_{0Y} > \nu_{0X} \), the y-intercept for metal Y will be lower than that for metal X. ### Step 4: Conclusion The graph that illustrates the expected results will show: - Both lines having the same slope (indicating the same value of \( \frac{h}{e} \)). - The line for metal Y starting at a lower value on the V-axis (indicating a higher threshold frequency). ### Final Answer The correct graph will depict two straight lines with the same slope, where the line for metal Y is positioned lower than that for metal X on the V-axis. ---

To solve the problem regarding the photoelectric emission from metals X and Y, we need to analyze the relationship between the stopping potential (V) and the frequency (f) of the incident light. Here are the steps to arrive at the solution: ### Step 1: Understand the Work Function The work function (φ) of a metal is the minimum energy required to eject an electron from the surface of that metal. It is related to the threshold frequency (ν₀) by the equation: \[ \phi = h \nu_0 \] where \( h \) is Planck's constant. Given that metal Y has a greater work function than metal X, we can express this as: ...
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