Animated Solution for Physics - Dual Nature of Matter and Radiation: Assuming the nitrogen molecule is moving with rms velocity at 400 K, the de-Broglie wavelength of nitrogen molecule is close to
(Given, weight of N2 molecule =4.64×10−26 kg, Boltzmann constant =1.38×10−23 J/K and Planck's constant =6.63×10−34 J-s)
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Visualized Solution
The Moving Molecule
T=400 K
m=4.64×10−26 kg
de-Broglie Wavelength
λ=ph
K=23kT
p=2mK=3mkT
λ=3mkTh
Substituting Values
λ=3×1.38×10−23×400×4.64×10−266.63×10−34
Simplifying the Denominator
λ=7683.84×10−496.63×10−34
λ=768.384×10−486.63×10−34
Calculating Square Root
768.384≈27.72
λ=27.72×10−246.63×10−34
Final Wavelength
λ≈0.239×10−10 m
λ≈0.24A˚
Food for Thought
What if the gas was H2 instead of N2?
λ∝m1
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The Sigma Insight: Matter Waves and de Broglie Relation
Solution Diagram
Unveiling the Quantum Dance of a Nitrogen Molecule
Imagine a nitrogen molecule zipping around randomly in a container at 400 K. Classical physics tells us it's just a tiny particle bouncing off walls. But quantum mechanics, specifically Louis de Broglie's brilliant hypothesis, reveals a deeper truth: every moving particle has a wave associated with it.
This isn't just a mathematical trick; it's the fundamental nature of reality. The faster the particle moves, or the heavier it is, the shorter its wavelength. Today, we are going to calculate the exact wavelength of this microscopic quantum dance.
The Master Equation
To find this wavelength, we start with the legendary de Broglie equation:
λ=ph
Here, h is Planck's constant and p is the momentum of the molecule. But we aren't given the momentum directly; we are given the temperature T. This is where the Kinetic Theory of Gases bridges the gap. For an ideal gas molecule, its average translational kinetic energy K is directly proportional to its absolute temperature:
K=23kT
We also know the classic relationship between kinetic energy and momentum: p=2mK. By substituting our expression for K into this momentum equation, we get:
p=2m(23kT)=3mkT
Now, we substitute this momentum back into our de Broglie equation to forge our master formula:
λ=3mkTh
Crunching the Numbers
This is where many students make silly mistakes. We have a beautiful formula, but the numbers are messy. Let's carefully substitute the given values:
λ=3×1.38×10−23×400×4.64×10−266.63×10−34
Let's tackle the denominator first. Ignore the powers of ten for a moment and multiply the coefficients: 3×1.38×400×4.64=7683.84.
Next, combine the powers of ten: 10−23×10−26=10−49. So, the term inside the square root is 7683.84×10−49.
Here is a pro-tip: Never try to take the square root of an odd power of ten. Shift the decimal point to make the exponent even. Let's rewrite it as 768.384×10−48.
The Final Reveal
Now, we need the square root of 768.384. We know 272=729 and 282=784. Since 768 is closer to 784, the square root will be roughly 27.7. The square root of 10−48 is simply 10−24.
λ=27.72×10−246.63×10−34
Dividing 6.63 by 27.72 gives approximately 0.239. Subtracting the exponents (−34−(−24)) leaves us with 10−10.
λ≈0.239×10−10 m
Since 10−10 m is exactly 1A˚ (Angstrom), we can elegantly write our final answer as:
λ≈0.24A˚
And there you have it! The quantum wavelength of a nitrogen molecule at room temperature is roughly a quarter of an Angstrom—smaller than the size of an atom itself. Keep practicing these calculations, and the math will become second nature!