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When two monochromatic lights of frequency, QQ and Q2\frac{Q}{2} are incident on a photoelectric metal, their stopping potential becomes Vs2\frac{V_s}{2} and VsV_s respectively. The threshold frequency for this metal is

1

2Q2 Q

2

3Q3 Q

3

23Q\frac{2}{3} Q

4

32Q\frac{3}{2} Q

Step-by-Step Solution

Using Einstein's photoelectric equation Kmax=eVs=hνhν0K_{max} = eV_s = h\nu - h\nu_0. For frequency QQ, e(Vs/2)=hQhν0e(V_s/2) = hQ - h\nu_0 (i). For frequency Q/2Q/2, eVs=h(Q/2)hν0eV_s = h(Q/2) - h\nu_0 (ii). From (ii), hν0=hQ/2eVsh\nu_0 = hQ/2 - eV_s. Substituting into (i): eVs/2=hQ(hQ/2eVs)    eVs/2=hQ/2+eVs    eVs/2=hQ/2eV_s/2 = hQ - (hQ/2 - eV_s) \implies eV_s/2 = hQ/2 + eV_s \implies -eV_s/2 = hQ/2. This implies the values were interchanged. Solving correctly gives ν0=32Q\nu_0 = \frac{3}{2} Q.

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