Animated Solution for Physics - Dual Nature of Matter and Radiation: The de-Broglie wavelength associated with an electron and a proton were calculated by accelerating them through same potential of 100 V. What should nearly be the ratio of their wavelengths? (mp=1.00727 u, me=0.00055 u)
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Visualized Solution
Visualizing the Setup
Electron and proton accelerated by ΔV=100 V
de-Broglie Wavelength Formula
λ=ph=2mKh
K=qV⟹λ=2mqVh
Identifying Constants
h is Planck’s constant
V=100 V (same for both)
qe=qp=e (same magnitude)
Wavelength-Mass Relation
λ∝m1
Ratio of Wavelengths
λpλe=memp
Substituting Mass Values
λpλe=0.00055 u1.00727 u
Calculating the Mass Ratio
memp=55100727≈1831.4
Final Wavelength Ratio
λpλe=1831.4≈42.79≈43
λe:λp=43:1
Independence from Potential
The ratio λpλe is independent of V.
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The Sigma Insight: Matter Waves and de Broglie Relation
Solution Diagram
The Dance of Matter Waves
Electron vs. Proton
Imagine an electron and a proton, both standing at the starting line of a particle accelerator. We flip the switch, applying a potential difference of 100 V. The electron darts towards the positive plate, while the proton lumbers towards the negative plate. As they accelerate, they gain kinetic energy, and according to quantum mechanics, they begin to exhibit wave-like properties. But whose wave is longer? Let's dive into the mathematics of matter waves to find out.
The Master Equation
To find the ratio of their de-Broglie wavelengths, we need a formula that connects the wavelength λ to the accelerating potential V. We start with the fundamental de-Broglie relation:
λ=ph
We know that the momentum p is related to kinetic energy K by p=2mK. Furthermore, the kinetic energy gained by a particle of charge q accelerated through a potential V is K=qV. Substituting this into our momentum equation gives us the master equation for this problem:
λ=2mqVh
The Beauty of Ratios
Now, let's look closely at this formula and identify the constants for our specific scenario. Planck's constant h is a universal constant. The accelerating potential V is given as 100 V for both particles. Finally, the magnitude of the charge q is identical for both an electron and a proton (qe=qp=e).
Since h, q, and V are all constant, we can establish a beautiful proportionality. The de-Broglie wavelength is inversely proportional to the square root of the particle's mass:
λ∝m1
This tells us intuitively that the heavier the particle, the shorter its wavelength. Because we want the ratio of the electron's wavelength to the proton's wavelength, we can set up the following relation:
λpλe=memp
The Final Computation
Now comes the execution phase. We substitute the given mass values into our ratio equation. The mass of the proton is mp=1.00727 u, and the mass of the electron is me=0.00055 u. Notice that we don't need to convert atomic mass units (u) to kilograms because the units will perfectly cancel out in the ratio.
λpλe=0.000551.00727
To make the division easier, we can shift the decimal point five places to the right for both numbers:
memp=55100727≈1831.4
Finally, we need to find the square root of 1831.4. We can estimate this by recalling perfect squares: 402=1600 and 452=2025. Our number is roughly in the middle, slightly closer to 1600. If we test 432, we get 1849, which is incredibly close to 1831.4.
λpλe=1831.4≈42.79
Rounding to the nearest integer, we get 43. Therefore, the ratio of their wavelengths is 43:1.
A Fascinating Takeaway: Did you notice that the 100 V potential completely vanished from our calculation? This means whether you accelerate these particles with 100 V, 1000 V, or a million volts, the ratio of their de-Broglie wavelengths will always remain 43:1. It is an intrinsic property dictated solely by the ratio of their masses!