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Question: A monochromatic source of light operating at 200W emits \( 4 \times {10^{20}} \) photons per second....

A monochromatic source of light operating at 200W emits 4×10204 \times {10^{20}} photons per second. Find the wavelength of the light (in ×107m\times {10^{ - 7}}m )

Explanation

Solution

Using Planck’s energy-frequency relation we have to find the energy of a single photon in terms of wavelength. Multiplying it with the total number of photons emitted per second gives us the total energy emitted per second. Since we are given the photons emitted per second, the energy will be equal to power.

Formula used
EP=h×cλ{E_P} = \dfrac{{h \times c}}{\lambda } , where Ep{E_p} the energy of a single photon is, λ\lambda is the wavelength of light in meters , cc is the speed of light in free space and hh is the Planck’s constant.
P=EtP = \dfrac{E}{t} , EE denotes power, EE is represented by energy and tt denotes time.
ETotal=n×Ep{E_{Total}} = n \times {E_p} ETotal{E_{Total}} represents the total energy, nn denotes the number of photons and Ep{E_p} is the energy of photon.

Complete step-by-step answer:
We know from Planck’s energy-frequency relation that EP=hν{E_P} = h\nu where Ep{E_p} is the energy of photon (also known as photon energy), hh is the Planck’s constant whose value is 6.626×1034J.s6.626 \times {10^{ - 34}}J.s in SI units and ν\nu is the frequency of the wave. Also note that the frequency of a wave can be expressed in terms of its wavelength and speed. This is given by the equation ν=cλ\nu = \dfrac{c}{\lambda } .Here cc is the speed of light ( 3×108m/s3 \times {10^8}m/s ) and λ\lambda is the wavelength. Substituting this equation in Planck’s energy-frequency relation we get
EP=h×cλ{E_P} = \dfrac{{h \times c}}{\lambda } .
EP=6.626×1034×3×108λ{E_P} = \dfrac{{6.626 \times {{10}^{ - 34}} \times 3 \times {{10}^8}}}{\lambda }
Since t=1st = 1s , according to the equation P=EtP = \dfrac{E}{t} we get P=EP = E .Given P=200WP = 200W .
P=EP = E
Using equation ETotal=n×Ep{E_{Total}} = n \times {E_p} , we get
P=ETotal=n×EpP = {E_{Total}} = n \times {E_p}
Here the number of photons per second is given. n=4×1020n = 4 \times {10^{20}} .
200=4×1020×Ep200 = 4 \times {10^{20}} \times {E_p}
Substituting EP=6.626×1034×3×108λ{E_P} = \dfrac{{6.626 \times {{10}^{ - 34}} \times 3 \times {{10}^8}}}{\lambda } .
200=4×1020×6.626×1034×3×108λ200 = 4 \times {10^{20}} \times \dfrac{{6.626 \times {{10}^{ - 34}} \times 3 \times {{10}^8}}}{\lambda }
λ=4×1020×6.626×1034×3×108200\lambda = \dfrac{{4 \times {{10}^{20}} \times 6.626 \times {{10}^{ - 34}} \times 3 \times {{10}^8}}}{{200}}
λ=4×107m\lambda = 4 \times {10^{ - 7}}m

Note: When light of a certain minimum frequency hits the metal surface the electrons will be just ejected. This minimum frequency required is called threshold frequency ν0{\nu _0} . .The value hν0h{\nu _0} is called the work function. This work function varies according to each metal surface. The light falling on the metal surface therefore should be greater than the threshold frequency.
If electromagnetic radiation of frequency ν\nu which is greater than the threshold frequency falls on the metal surface the additional energy will be given to the electron as kinetic energy. This can be written in equation form as hν=hν0+KEh\nu = h{\nu _0} + KE . Here KE represents the kinetic energy.