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Question
Following results are observed when sodium metal is irradiated with different wavelengths. Calculate (a) threshold wavelength and, (b) Planck’s constant.
λ (nm) | 500 | 450 | 400 |
v × 10-5 (cm s-1) | 2.55 | 4.35 | 5.35 |
Solution 1
Assuming the threshold wavelength to be `lambda_0 " nm"(= lambda_0 xx 10^(-9)" m")`, the kinetic energy of the radiation is given as:
`"h" ("v" - "v"_0) = 1/2 " mv"^2` ...........(i)
Since v = `"c" / λ`, the equation (i) can write the following types-
`"hc" [1/λ - 1/λ_0] = 1/2 "mv"^2` ..............(ii)
Upon replacing the results given by the three experiments in the equation (ii),
`"hc"/10^-9 [1/500 - 1/λ_0] = 1/2 "m" xx (2.55 xx 10^6)^2` .......(iii)
`"hc"/10^-9 [1/450 - 1/λ_0] = 1/2 "m" xx (4.35 xx 10^6)^2` .....…(iv)
`"hc"/10^-9 [1/400 - 1/λ_0] = 1/2 "m" xx (5.35 xx 10^6)^2` ........…(v)
Dividing equation (iv) by equation (iii)
`(λ_0 - 450)/(450 λ_0) xx (500 λ_0)/(λ_0 - 500) = [4.35/2.55]^2`
or `(λ_0 - 450)/(λ_0 - 500) = [4.35/2.55]^2 xx 450/500` = 2.619
or λ0 − 450 = 2.619 λ0 − (500 × 2.619)
or 1.619 λ0 = 1309.5 − 450 = 859.5
or λ0 = `859.5/1.619` = 530.88 = 531 nm
The value of the Planck’s constant is H, the value of the λ0 can be obtained on replacing in one of the three classes.
Solution 2
Let the threshold wavelength to be λ0 nm = λ0×10-9 m .
Following equation holds true for photoelectric emission in given case:
K.E. = 1/2 mv2 = h(ν - ν0)
⇒1/2 mv2 = hν - hν0
⇒ hν0 = hν - 1/2 mv2
⇒ hc/λ0 = hc/λ - 1/2 mv2
`=> lambda_0 = 1/(1/lambda - 1/2 m/hc v^2) = 1/(1/lambda - 1/2 (9.1xx10^(-31))/(6.6xx10^(-34)xx3xx10^8))v^2`
a) Substituting the value of λ and v from the above given data, we get three values of λ0 as,
λ0(1) = 541 nm
λ0(2) = 546 nm
λ0(3) = 542 nm
Threshold frequency = λav = {λ0(1)+λ0(2)+λ0(3)}/3 = (541+546+542)/3 = 543 (approx 540)
Notes
Note: part (b) of the question is not done due to the incorrect values of velocity given in the question
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