Sub in $(1)$: $K_1=\dfrac{K_2+\phi}{2}-\phi=\dfrac{K_2}{2}-\dfrac{\phi}{2}$
$2K_1=K_2-\phi\Rightarrow\phi=K_2-2K_1$
📘 Einstein's Photoelectric Equation
$K_{max}=hc/\lambda-\phi$. Two equations eliminate $hc/\lambda_2$. The substitution $hc/\lambda_1=hc/(2\lambda_2)=(K_2+\phi)/2$ leads directly to $\phi=K_2-2K_1$.
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Important Concepts
λ₁=2λ₂ Means E₁=E₂/2E=hc/λ. Longer λ → less energy. E₁=hc/(2λ₂)=E₂/2.
Elimination StrategyExpress both KEs in terms of hc/λ₂ and φ. Eliminate hc/λ₂ to get φ.
Result φ=K₂−2K₁2K₁=K₂−φ → φ=K₂−2K₁.
Physical CheckK₁λ₂). φ>0 requires K₂>2K₁.
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FAQs
1
Why E₁=E₂/2 when λ₁=2λ₂?
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E=hc/λ: doubling λ halves E.
2
Can φ be negative?
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No. Work function must be positive. K₂>2K₁ is required.
3
Typical work function values?
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Metals: 2−5 eV. Cesium: ~2.1eV. Gold: ~5.1eV.
4
What if K₁=0?
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φ=K₂−0=K₂. Light of λ₁ is at threshold, λ₂=λ₁/2 gives K₂=φ.