The work functions of cesium (Cs) and lithium (Li) metals are 1.9 eV and 2.5 eV, respectively. If we incident a light of wavelength 550 nm on these two metal surface, then photo-electric effect is possible for the case of: (1) Li only (2) Cs only (3) Neither Cs nor Li (4) Both Cs and Li

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Published July 8, 2025
Physics
Modern Physics
Photoelectric Effect
Work Function
Photon Energy

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Detailed Explanation

Key Concepts

  1. Photon Energy Formula
    Every photon has energy E=hcλE = \frac{hc}{\lambda} where:

    • h=6.626×1034J\cdotpsh = 6.626\times10^{-34}\,\text{J·s} (Planck’s constant)
    • c=3.0×108m/sc = 3.0\times10^{8}\,\text{m/s} (speed of light)
    • λ\lambda is the wavelength in metres
  2. Work Function (ϕ)(\phi)
    The minimum energy a photon must have to eject an electron from a metal surface.

  3. Condition for Photo-Emission
    A photon can eject an electron if EphotonϕE_{\text{photon}} \geq \phi

  4. Comparing Numbers
    Convert photon energy into the same unit (eV) as the work function, then compare.

Logical Flow to Solve

  • Convert the given wavelength (550 nm) to energy using the formula.
  • Translate that energy from joules to electron-volts.
  • Compare the resulting energy (≈2.25 eV) with each metal’s work function.
  • Conclude which metals meet the criterion EphotonϕE_{\text{photon}} \geq \phi.

Simple Explanation (ELI5)

What’s Happening?

Imagine you have two locked doors—one needs a lighter push to open (Cesium) and the other needs a harder push (Lithium). A flashlight beam is like a stream of energy pushes. If the push is strong enough, the door opens and an electron pops out.

Numbers in Simple Words

  • Cesium’s lock needs 1.9 energy coins (eV).
  • Lithium’s lock needs 2.5 energy coins (eV).
  • The yellowish light we shine (550 nm) carries about 2.25 energy coins each.

Who Opens?

  • Cesium: needs 1.9 coins, light gives 2.25 → door opens!
  • Lithium: needs 2.5 coins, light gives 2.25 → not enough, door stays shut.

So only Cesium lets electrons out.

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Step-by-Step Solution

Step 1: Photon Energy for 550 nm

Convert 550 nm to metres: λ=550nm=550×109m\lambda = 550\,\text{nm} = 550\times10^{-9}\,\text{m}

Calculate energy in joules: E=hcλ=(6.626×1034)(3.0×108)550×109E = \frac{hc}{\lambda} = \frac{(6.626\times10^{-34})(3.0\times10^{8})}{550\times10^{-9}} E3.61×1019JE \approx 3.61\times10^{-19}\,\text{J}

Step 2: Convert to Electron-Volts

1eV=1.602×1019J1\,\text{eV} = 1.602\times10^{-19}\,\text{J} E=3.61×10191.602×10192.25eVE = \frac{3.61\times10^{-19}}{1.602\times10^{-19}} \approx 2.25\,\text{eV}

Step 3: Compare with Work Functions

  • Cesium: ϕCs=1.9eV\phi_{\text{Cs}} = 1.9\,\text{eV}
    2.25eV1.9eV        Photo-electron emitted2.25\,\text{eV} \ge 1.9\,\text{eV} \;\;\rightarrow\;\; \text{Photo-electron emitted}
  • Lithium: ϕLi=2.5eV\phi_{\text{Li}} = 2.5\,\text{eV}
    2.25eV<2.5eV        No emission2.25\,\text{eV} < 2.5\,\text{eV} \;\;\rightarrow\;\; \text{No emission}

Final Answer

Only Cesium exhibits the photo-electric effect.
Option (2) — Cs only

Examples

Example 1

Solar panels use materials with low work functions so that sunlight photons can easily knock out electrons and create current.

Example 2

Photo cells in street lights often use Cesium or Potassium because their low work functions allow visible light to trigger switching.

Example 3

In night-vision devices, Gallium Arsenide cathodes are chosen so that near-infrared photons have just enough energy to release electrons.

Example 4

Ultraviolet cleanup lamps can ionise surfaces where even very high work-function metals lose electrons under UV exposure.

Visual Representation

References

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