Imagine you are trying to knock a heavy ball out of a ditch. You can throw a million ping-pong balls at it, but it won't budge. However, a single, fast-moving bowling ball will knock it right out. This is the essence of the photoelectric effect!
The Condition for Photoemission
For an electron to escape the metallic surface, it needs a minimum amount of energy called the work function (ϕ)
The incident light provides this energy in discrete packets called photons. The energy of a photon is given by E=λhc.
Notice the inverse relationship: a smaller wavelength (
λ) means a higher energy (
E). The maximum wavelength that can just barely eject an electron is called the
threshold wavelength (
λ0). For emission to occur, our incident light must have a wavelength strictly less than this threshold:
λ<λ0
Analyzing the Spectrum
In our problem, the threshold wavelength is given as λ0=5200 A˚
This value sits comfortably in the visible spectrum (around the green region).
Now, let's look at our options:
1. Infrared (IR) Light: Infrared radiation has a longer wavelength than visible light, typically λIR>7000 A˚. Since λIR>5200 A˚, its photons are like the ping-pong balls—they simply don't have enough energy to eject an electron.
2. Ultraviolet (UV) Light: Ultraviolet radiation has a shorter wavelength than visible light, typically λUV<4000 A˚. Since λUV<5200 A˚, its photons are the bowling balls! They pack more than enough energy to cause photoemission.
Does Power Matter?
You might be wondering about the 50 W and 1 W ratings
The power of the lamp tells us about the intensity of the light—how many photons are emitted per second.
A 50 W infrared lamp shoots a massive number of low-energy photons, but none of them can eject an electron. A 1 W ultraviolet lamp shoots fewer photons, but every single one has enough energy to knock an electron out.
Therefore, both the 50 W and 1 W ultraviolet lamps will successfully cause photoelectric emission. The 50 W UV lamp will just eject more electrons per second than the 1 W UV lamp!