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From the above figure the values of stop...

From the above figure the values of stopping potentials for `M_(1)` and `M_(2)` for a frequency `v_(3)( gt v_(02))` of the incident radiatioins are `V_(1)` and `V_(2)` respectively. Then the slope of the line is equal to

A

`(V_(2)-V_(1))/(v_(02)-v_(01))`

B

`(V_(1)-V_(2))/(v_(02)-v_(01))`

C

`(V_(2))/(v_(02)-v_(01))`

D

`(V_(1))/(v_(02)-v_(01))`

Text Solution

Verified by Experts

`hv_(01) + eV_(1) = hv_(02) + eV_(2)`
`e(V_(1) - V_(2)) = h (V_(02) - V_(01)) ,(h)/(e ) = ((V_(1)-V_(2)))/((V_(02)-V_(01))`
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NARAYNA-DUAL NATURE OF RADIATION AND MATTER-EXERCISE - 4
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