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Question: The graph between\(\dfrac{1}{\lambda }\) and stopping potential \((V)\) of three metals having work ...

The graph between1λ\dfrac{1}{\lambda } and stopping potential (V)(V) of three metals having work functions ϕ1,ϕ2{{\phi }_{1,}}{{\phi }_{2}} and ϕ3{{\phi }_{3}} in an experiment of photo-electric effect is plotted as shown in the figure. Which of the following statement(s) is/are correct?[ Here λ\lambda is the wavelength of the incident ray].

A. Ratio of work functions ϕ1:ϕ2:ϕ3=1:2:4{{\phi }_{1}}:{{\phi }_{2}}:{{\phi }_{3}}=1:2:4
B. Ratio of work functions ϕ1:ϕ2:ϕ3=4:2:1{{\phi }_{1}}:{{\phi }_{2}}:{{\phi }_{3}}=4:2:1
C.tanθ\tan \theta is directly proportional to hce\dfrac{hc}{e} ,where hh is Planck’s constant and cc is the speed of light.
D. The violet colour light can eject photoelectrons from metal 22 and 33

Explanation

Solution

Here we will use Einstein’s photoelectric equation. From that equation we will see how the graph between stopping potential and 1λ\dfrac{1}{\lambda } gives information about different parameters. From that information we will be able to answer the question. We follow these steps to answer the question.

Formula used: V0=(hce)1λ(hce)1λ0{{V}_{0}}=(\dfrac{hc}{e})\dfrac{1}{\lambda }-(\dfrac{hc}{e})\dfrac{1}{{{\lambda }_{0}}}

Complete step by step answer:
If V0{{V}_{0}} is the stopping potential,λ\lambda is the wavelength of the incident light andλ0{{\lambda }_{0}} is the threshold wavelength then Einstein’s photoelectric equation can be re written as
V0=(hce)1λ(hce)1λ0.....(1){{V}_{0}}=(\dfrac{hc}{e})\dfrac{1}{\lambda }-(\dfrac{hc}{e})\dfrac{1}{{{\lambda }_{0}}}.....(1)
If we compare this equation with the equation of a straight line
y=mx+cy=mx+c then we can see the slope of the graph m=(hce)m=(\dfrac{hc}{e}) . Now from the question the slope of the graph is tanθ\tan \theta , so tanθ=hce\tan \theta =\dfrac{hc}{e} .
Thus the option C is correct.
Again the equation (1)(1) can be re written as
eV0=hcλϕ........(2)e{{V}_{0}}=\dfrac{hc}{\lambda }-\phi ........(2) , where ϕ\phi is the work function of the metal. Now when V0=0{{V}_{0}}=0 , we can write from (2)(2)
ϕ=hcλ orϕ1λ \begin{aligned} & \phi =\dfrac{hc}{\lambda } \\\ & or\phi \propto \dfrac{1}{\lambda } \\\ \end{aligned}
Now from the graph we have
1λ1:1λ2:1λ3=0.001:0.002:0.004=1:2:4 orϕ1:ϕ2:ϕ3=1:2:4 \begin{aligned} & \dfrac{1}{{{\lambda }_{1}}}:\dfrac{1}{{{\lambda }_{2}}}:\dfrac{1}{{{\lambda }_{3}}}=0.001:0.002:0.004=1:2:4 \\\ & or{{\phi }_{1}}:{{\phi }_{2}}:{{\phi }_{3}}=1:2:4 \\\ \end{aligned}
So the option A is correct.
Now violet has the wavelength
λv=380nm or1λv=0.0026nm1 \begin{aligned} & {{\lambda }_{v}}=380nm \\\ & or\dfrac{1}{{{\lambda }_{v}}}=0.0026n{{m}^{-1}} \\\ \end{aligned}
Thus from the graph we can see 1λv>1λ2\dfrac{1}{{{\lambda }_{v}}}>\dfrac{1}{{{\lambda }_{2}}} and1λv<1λ3\dfrac{1}{{{\lambda }_{v}}}<\dfrac{1}{{{\lambda }_{3}}}, so violet light can eject electron from metal 22 but not from metal 33 .
So option D is also incorrect.

So, the correct answer is “Option A and C”.

Note: Here we need to know about the photoelectric effect. We need to modify Einstein's photoelectric equation in different forms according to the question to be answered. An incident radiation can only eject electrons from a metal if its frequency is greater than some minimum value called the threshold frequency.