In photoelectric effect- the slope of the straight line graph between stopping potential and frequency of the incident light gives the ratio of Planck-s constant toWork functionK-E- of electronCharge of electronPhotoelectric current

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Hv-hv0-K-Eat stopping potential K-E-eV-x21D2-hv-hv0-eVV-he-v-x2212-v0-The slope of graph b-w stopping potential and frequency is he- where e is charge of-xA0- electron-

In photoelectric effect, the slope of the straight line graph between stopping potential and frequency of the incident light gives the ratio of Planck's constant to
Work function
K.E. of electron
Charge of electron
Photoelectric current

$h v = h v_{0} + K . E$
at stopping potential K.E $=$ eV
$\Rightarrow h v = h v_{0} + e V$

$V = \frac{h}{e} (v - v_{0})$

The slope of graph b/w stopping potential and frequency is $\frac{h}{e}$ , where e is charge of electron.

In photoelectric effect, the slope of the straight line graph between stopping potential and frequency of the incident light gives the ratio of Planck's constant toWork functionK.E. of electronCharge of electronPhotoelectric current

hv=hv0+K.Eat stopping potential K.E=eV⇒hv=hv0+eVV=he(v−v0)The slope of graph b/w stopping potential and frequency is he, where e is charge of electron.

In photoelectric effect, the slope of the straight line graph between stopping potential and frequency of the incident light gives the ratio of Planck's constant to
Work function
K.E. of electron
Charge of electron
Photoelectric current

$h v = h v_{0} + K . E$
at stopping potential K.E $=$ eV
$\Rightarrow h v = h v_{0} + e V$

$V = \frac{h}{e} (v - v_{0})$

The slope of graph b/w stopping potential and frequency is $\frac{h}{e}$ , where e is charge of electron.