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Exercises · 11.4

Q.Monochromatic light of wavelength 632.8 nm632.8\ \text{nm} is produced by a helium-neon laser. The power emitted is 9.42 mW9.42\ \text{mW}.

(a) Find the energy and momentum of each photon in the light beam,
(b) How many photons per second, on the average, arrive at a target irradiated by this beam? (Assume the beam to have uniform cross-section which is less than the target area), and
(c) How fast does a hydrogen atom have to travel in order to have the same momentum as that of the photon?
Puducherry CbseNCERTSubjective· 3mImportance★★★★★
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The problem connects photon energy, momentum, and number flux to macroscopic laser power. Each photon carries energy E=hc/λE = hc/\lambda and momentum p=h/λp = h/\lambda; the number of photons per second is power divided by photon energy; and the hydrogen atom’s speed for equal momentum comes from p=mHvp = m_\text{H} v.


Concept and Intuition

A laser beam is a stream of photons. Even though the beam looks continuous, its power is the sum of the energies of individual photons arriving per second. Each photon, being a quantum of light, has energy proportional to its frequency and momentum inversely proportional to its wavelength — a direct consequence of de Broglie’s relation and Planck’s law.

The key is to treat the macroscopic power (9.42 mW9.42\ \text{mW}) as the product of the number of photons per second and the energy per photon. For part (c), we simply equate the photon’s momentum to the classical momentum of a hydrogen atom and solve for its speed.


Step-by-step solution

1. Photon energy from wavelength

The energy of a single photon is given by the Planck-Einstein relation:

E=hf=hcλE = h f = \frac{h c}{\lambda}

where

h=6.626×10−34 J⋅sh = 6.626 \times 10^{-34}\ \text{J·s} (Planck’s constant),

c=3.00×108 m/sc = 3.00 \times 10^{8}\ \text{m/s},

λ=632.8 nm=632.8×10−9 m\lambda = 632.8\ \text{nm} = 632.8 \times 10^{-9}\ \text{m}.

Substitute:

E=(6.626×10−34)(3.00×108)632.8×10−9E = \frac{(6.626 \times 10^{-34})(3.00 \times 10^{8})}{632.8 \times 10^{-9}}

First compute numerator: 6.626×3.00=19.8786.626 \times 3.00 = 19.878, so 19.878×10−26 J⋅m19.878 \times 10^{-26}\ \text{J·m}.

Divide by 632.8×10−9632.8 \times 10^{-9}:

E=19.878×10−26632.8×10−9=19.878632.8×10−17E = \frac{19.878 \times 10^{-26}}{632.8 \times 10^{-9}} = \frac{19.878}{632.8} \times 10^{-17}

19.878632.8≈0.03141\frac{19.878}{632.8} \approx 0.03141, so

E≈3.141×10−19 JE \approx 3.141 \times 10^{-19}\ \text{J}

Tip

A quick check: visible photons have energies around 10−19 J10^{-19}\ \text{J}, so this result is reasonable.

2. Photon momentum

For a photon, momentum is:

p=hλp = \frac{h}{\lambda}

Substitute:

p=6.626×10−34632.8×10−9=6.626632.8×10−25p = \frac{6.626 \times 10^{-34}}{632.8 \times 10^{-9}} = \frac{6.626}{632.8} \times 10^{-25}

6.626632.8≈0.01047\frac{6.626}{632.8} \approx 0.01047, so

p≈1.047×10−27 kg⋅m/sp \approx 1.047 \times 10^{-27}\ \text{kg·m/s}

Watch out

Do not use p=E/cp = E/c here unless you keep units consistent — it gives the same result but is one extra step. The direct h/λh/\lambda is simpler.

3. Number of photons per second

Power P=9.42 mW=9.42×10−3 J/sP = 9.42\ \text{mW} = 9.42 \times 10^{-3}\ \text{J/s}.

If each photon carries energy EE, then the number of photons arriving per second is:

n=PEn = \frac{P}{E}

Substitute:

n=9.42×10−33.141×10−19n = \frac{9.42 \times 10^{-3}}{3.141 \times 10^{-19}} …

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