Q.A microscope using suitable photons is employed to locate an electron in an atom within a distance of 0.1 Å. What is the uncertainty involved in the measurement of its velocity?
Concept understanding — De Broglie Wavelength
De Broglie Wavelength: When Particles Start Acting Like Waves
Imagine you're holding a cricket ball. You know exactly where it is, and if you throw it, you can predict its path. That's a particle — localised, definite, following Newton's laws. Now think of light. You can't "hold" a beam of light; it spreads out, bends around corners, creates interference patterns. That's a wave — spread out, not localised.
For centuries, physics kept these two worlds separate. Particles were particles. Waves were waves. Never the twain shall meet.
Then came a young French physicist, Louis de Broglie, in 1924. He asked a question that seemed almost absurd: If light — which we thought was a wave — can behave like a particle (the photoelectric effect), then why can't a particle — say, an electron — behave like a wave?
That question turned physics upside down.
The Core Idea
De Broglie proposed that every moving particle has a wave associated with it. The wavelength of that wave depends on the particle's momentum. The faster or heavier the particle, the shorter the wavelength.
λ=ph=mvh
Where:
- λ = de Broglie wavelength (in metres)
- h = Planck's constant (6.626×10−34 J⋅s)
- p = momentum of the particle (mv for non-relativistic speeds)
This is not a mathematical trick. It's a physical reality. An electron moving through a crystal actually behaves like a wave of this wavelength — it can diffract, interfere, and form patterns just like light does.
Why You Don't See It in Daily Life
Here's the crucial point: the de Broglie wavelength is incredibly tiny for everyday objects.
Take a cricket ball of mass 0.16 kg moving at 30 m/s. Its de Broglie wavelength is:
λ=0.16×306.626×10−34≈1.38×10−34 m
That's about a hundred trillion trillion times smaller than the nucleus of an atom. No experiment can detect such a wave — it's effectively zero for all practical purposes.
Now take an electron (mass 9.1×10−31 kg) accelerated through 100 volts. Its speed is about 5.9×106 m/s. Its de Broglie wavelength:
λ=9.1×10−31×5.9×1066.626×10−34≈1.23×10−10 m
That's about 0.12 nanometres — comparable to the spacing between atoms in a crystal. This is measurable. And indeed, in 1927, Davisson and Germer fired electrons at a nickel crystal and observed diffraction — the unmistakable signature of a wave.
The de Broglie wavelength is only observable when it is comparable to the size of objects the particle interacts with. For macroscopic objects, it's far too small to matter. For subatomic particles, it's the key to understanding their behaviour.
What This Means Physically
The wave is not a physical wave in space like a water wave. It's a probability wave — its amplitude at any point tells you the probability of finding the particle there. Where the wave amplitude is large, you're likely to find the particle; where it's zero, you won't.
This wave-particle duality is not a compromise. It's the actual nature of reality. An electron is neither a pure particle nor a pure wave — it's something that shows particle-like behaviour in some experiments (like hitting a screen at a point) and wave-like behaviour in others (like passing through two slits and interfering with itself).
De Broglie's hypothesis is not just a clever idea — it's the foundation of quantum mechanics. Every particle has a wavelength, and that wavelength determines how it moves, where it can be found, and even why electrons in atoms occupy only certain discrete energy levels (standing waves around the nucleus).
A Quick Way to Remember
For an exam, you'll often need to compute the de Broglie wavelength of an electron accelerated through a potential difference V volts. The kinetic energy gained is eV, so:
21mv2=eV⇒v=m2eV
Substituting into λ=h/(mv) gives:
λ=2meVh
Plug in the numbers (h, me, e) and you get a handy formula:
For an electron accelerated through V volts:
λ(in A˚)=V12.27
So a 100 V electron has λ≈1.23 A˚ — right in the X-ray range.
The Bottom Line
De Broglie wavelength is the bridge between the particle and wave pictures of matter. It tells you that momentum and wavelength are two sides of the same coin. For large objects, the wavelength is negligible — Newtonian physics works fine. For tiny particles, the wavelength dominates — and you must use quantum mechanics.
When you see λ=h/p, remember: that's nature saying that everything — from electrons to planets — has a wave nature. It's just that for most things, the wave is too small to notice.
Searches like "de Broglie wavelength formula and examples" and "dual nature of matter class 12 physics" are very common, since this concept is central to the Dual Nature of Radiation and Matter chapter of the NCERT/CBSE Class 12 Physics curriculum. The handy λ=12.27/V shortcut for accelerated electrons is a frequent JEE Main and NEET numerical question.
Why this formula?
De Broglie Wavelength: Why the Formula Holds
Let's build this from the ground up — understanding why matter has a wavelength, not just memorizing λ=ph.
The Core Insight: Nature's Symmetry
Before de Broglie, physics had two separate worlds:
- Light — showed wave behaviour (diffraction, interference) but also particle behaviour (photoelectric effect)
- Matter — showed particle behaviour (momentum, collisions) but no wave behaviour yet
De Broglie asked a daring question in his 1924 PhD thesis:
If light (a wave) can behave like a particle, why can't a particle (like an electron) behave like a wave?
Nature should be symmetric — what applies to one should apply to the other.
Step 1: Start with Light (What We Already Knew)
For a photon, Einstein had given us two key relations:
- Energy: E=hf (Planck's relation)
- Momentum: p=λh (from E=pc for light, combined with c=fλ)
So for light:
λ=ph
This was experimentally verified for photons.
Step 2: De Broglie's Bold Hypothesis
De Broglie said: This relation is not special to light. It is universal.
For any particle with momentum p:
λ=ph
Where:
- λ = de Broglie wavelength
- h = Planck's constant (6.626×10−34 J⋅s)
- p = momentum of the particle
Step 3: Why Momentum and Not Velocity?
This is crucial. The formula uses momentum (p=mv), not just velocity.
For a non-relativistic particle (slow compared to light):
λ=mvh
For a relativistic particle (like an electron at high speed):
p=γmvwhereγ=1−v2/c21
λ=γmvh
Why momentum? Because momentum is the more fundamental quantity — it's conserved, it's frame-independent in a deeper sense, and it connects directly to the wave's phase.
Step 4: The Deeper Reasoning — Wave-Particle Duality
De Broglie didn't just guess. He reasoned:
- Every moving particle has an associated wave — called the "matter wave" or "pilot wave"
- The frequency of this wave comes from energy: f=hE
- The wavelength comes from momentum: λ=ph
These two relations are linked by the phase velocity of the wave:
vphase=fλ=hE⋅ph=pE
For a free particle with kinetic energy E=2mp2:
vphase=2mp=2v
This is half the particle's speed — a strange but mathematically consistent result.
Step 5: Experimental Confirmation (Why We Believe It)
De Broglie's idea was confirmed when electrons showed wave behaviour:
- Davisson-Germer experiment (1927): Electrons scattered off a nickel crystal produced diffraction patterns — exactly like X-rays (waves!)
- The measured wavelength matched λ=h/p perfectly
This was Nobel Prize material — de Broglie won in 1929.
Key Takeaways for Exams
| Concept | Formula | When to Use |
|---|---|---|
| De Broglie wavelength | λ=ph | Always — fundamental definition |
| Non-relativistic | λ=mvh | For v≪c (most exam problems) |
| Relativistic | λ=γmvh | For v≈c (rare in school exams) |
| For an electron accelerated through V volts | λ=2meVh | Derive from p=2mEk |
The Deeper "Why" — One Sentence
De Broglie wavelength exists because nature is symmetric: just as light has both wave and particle aspects, so must matter — and the bridge between them is Planck's constant h.
The formula λ=h/p is not derived from deeper principles — it is the fundamental postulate that connects the particle's momentum to its wave's wavelength. Its validity comes from experiment, not from pure mathematics.
The key idea is the Heisenberg Uncertainty Principle, which links the uncertainty in position (Δx) to the uncertainty in momentum (Δp). For an electron, momentum is p=mv, so an uncertainty in position forces a minimum uncertainty in velocity.
Step 1: Write the uncertainty principle:
Δx⋅Δp≥4πh
where h=6.63×10−34 J⋅s.
Step 2: Given Δx=0.1 A˚=0.1×10−10 m=10−11 m. For the minimum uncertainty, use the equality:
Δp=4πΔxh
Step 3: Since Δp=meΔv (mass of electron me=9.1×10−31 kg), the velocity uncertainty is:
Δv=4πmeΔxh
Step 4: Substitute values:
Δv=4×3.14×9.1×10−31×10−116.63×10−34
First compute denominator: 4×3.14≈12.56, then 12.56×9.1×10−31≈114.3×10−31=1.143×10−29, times 10−11 gives 1.143×10−40. So:
Δv≈1.143×10−406.63×10−34≈5.8×106 m/s
The uncertainty in velocity is 5.79×106 m s−1.
The Heisenberg Uncertainty Principle links the uncertainty in position to the uncertainty in momentum. Given Δx=0.1A˚, the minimum uncertainty in velocity is Δv≈5.8×106m/s.
The core idea here is the Heisenberg Uncertainty Principle — one of the most fundamental results in quantum mechanics. It says that you cannot simultaneously know both the position and the momentum of a particle with perfect precision. The more precisely you pin down where it is, the less precisely you can know how fast it's moving (and in which direction).
In this problem, a microscope "locates" an electron within a distance of 0.1A˚. That 0.1A˚ is the uncertainty in position, Δx. The principle then forces a minimum uncertainty in the electron's momentum, Δp, and from that we can find the uncertainty in velocity, Δv.
Let's walk through it step by step.
- State the Uncertainty Principle The Heisenberg Uncertainty Principle for position and momentum is:
Δx⋅Δp≥4πh
where h is Planck's constant (6.626×10−34J⋅s).
The ≥ sign means the product of the uncertainties can never be smaller than that value — it's a fundamental lower bound.
- Convert the given position uncertainty to metres The problem gives Δx=0.1A˚. Remember: 1A˚=10−10m. So:
Δx=0.1×10−10m=1×10−11m.
- Find the minimum uncertainty in momentum To get the smallest possible Δv, we take the equality case of the principle:
Δp=4πΔxh.
Plug in the numbers:
Δp=4×3.1416×1×10−116.626×10−34.
First, 4π≈12.5664.
Then:
Δp=12.5664×10−116.626×10−34=1.25664×10−106.626×10−34.
Divide:
Δp≈5.27×10−24kg⋅m/s.
- Relate momentum uncertainty to velocity uncertainty For an electron, momentum p=mv, where m is the electron's mass (9.11×10−31kg). Since the mass is known precisely, the uncertainty in momentum is directly related to the uncertainty in velocity:
Δp=mΔv⇒Δv=mΔp.
Substitute:
Δv=9.11×10−315.27×10−24.
That gives:
Δv≈5.78×106m/s.
- Interpret the result This is a huge speed — about 2% of the speed of light. It tells you that if you try to pin an electron's position down to the size of an atom (0.1 Å is roughly the diameter of a hydrogen atom), you lose almost all knowledge of its velocity. The electron could be moving anywhere from nearly stationary to millions of metres per second.
A common mistake is to forget that Δx must be in metres, not angstroms. Also, some students use Δp=h/Δx (the simpler form from some textbooks), but the correct quantum mechanical lower bound is h/4π. Using h/Δx would give an answer about 12 times smaller — still large, but wrong for this standard formulation.
Notice that the uncertainty in velocity is enormous compared to everyday speeds. This is why we can't talk about electrons "orbiting" like planets — the uncertainty principle smears out any definite path.
The minimum uncertainty in the electron's velocity is approximately 5.8×106m/s.
Showing the 12 most recent of 70 on this concept.
- CBSE 2026Set 55/1/11 markMCQQ.For questions 13 to 16, two statements are given – one labelled Assertion (A) and the other labelled Reason (R). Select the correct answer from the codes (A), (B), (C) and (D) below: (A) Both Assertion (A) and Reason (R) are true and Reason (R) is the correct explanation of the Assertion (A). (B) Both Assertion (A) and Reason (R) are true, but Reason (R) is not the correct explanation of the Assertion (A). (C) Assertion (A) is true, but Reason (R) is false. (D) Both Assertion (A) and Reason (R) are false. Assertion (A) : If accelerated electrons are passed through a narrow slit, a diffraction pattern is observed. Reason (R) : Electrons behave as both particles and waves.
›Reveal solutionSolution
Electrons exhibit wave-particle duality; their wave nature (de Broglie wavelength) causes diffraction when passing through narrow slits, just like light waves. Both statements are true, and the Reason correctly explains the Assertion.
Understanding Wave-Particle Duality
The heart of this question lies in one of quantum mechanics' most profound insights: matter at the atomic scale doesn't fit neatly into our classical categories of "particle" or "wave." Louis de Broglie proposed in 1924 that every moving particle has an associated wavelength, given by
λ=ph=mvh
where h is Planck's constant, p is momentum, m is mass, and v is velocity.
When we accelerate electrons, we increase their momentum. Yet even at high speeds, electrons retain a measurable de Broglie wavelength—typically on the order of angstroms for electrons accelerated through a few hundred volts. This wavelength is comparable to the spacing between atoms in crystals or the width of carefully engineered slits.
Examining the Assertion
Assertion (A): If accelerated electrons are passed through a narrow slit, a diffraction pattern is observed.
This is experimentally verified and true. The classic demonstration is the Davisson-Germer experiment (1927), which showed electron diffraction from crystal lattices. More dramatically, modern versions of the double-slit experiment with electrons—sending them one at a time—build up an interference pattern on a detector screen over time.
Diffraction occurs when waves encounter obstacles or apertures comparable to their wavelength. The electron beam, despite being composed of particles with mass and charge, produces the characteristic bright and dark fringes we associate with wave phenomena. The central maximum, secondary maxima, and minima all appear exactly as wave theory predicts.
For single-slit diffraction, minima occur at angles θ satisfying:
asinθ=nλ
where a is the slit width, n=1,2,3,…, and λ is the de Broglie wavelength.
Examining the Reason
Reason (R): Electrons behave as both particles and waves.
This is the principle of wave-particle duality, a cornerstone of quantum mechanics. It is unequivocally true.
Electrons exhibit particle properties: they have definite mass (9.11×10−31 kg), charge (−1.6×10−19 C), and produce localized impacts on detectors (you can count individual electron arrivals). Simultaneously, they exhibit wave properties: they diffract, interfere, and possess a wavelength and frequency.
Neither description alone is complete. The electron is a quantum object, and which aspect we observe depends on the experimental setup. When we look for particle behavior (measuring position or momentum), we find particles. When we create conditions for wave behavior (slits, crystals), we observe diffraction and interference.
TipA useful way to remember this: small wavelength (high momentum) → more particle-like behavior; large wavelength (low momentum) → more wave-like behavior. But both aspects are always present.
Connecting Assertion and Reason
Now the critical question: does the Reason explain the Assertion?
The answer is yes. The diffraction pattern observed when electrons pass through a slit is a direct consequence of their wave nature. Without wave-like behavior, electrons would simply pass through the slit in straight lines, creating a single bright spot on a screen—no fringes, no pattern.
The wave-particle duality is not just a parallel fact; it is the cause of the diffraction. The de Broglie wavelength associated with the electron's momentum determines the spacing and angular positions of the diffraction maxima and minima. The Reason provides the fundamental physical principle that makes the Assertion true.
Watch outDon't confuse "both are true" with "one explains the other." Many assertion-reason questions have two correct statements that are unrelated. Here, the causal link is explicit: wave nature → diffraction.
✓Final answerThe correct option is (A): Both Assertion and Reason are true, and Reason is the correct explanation of the Assertion.
- CBSE 2026Set 55/3/11 markMCQQ.A proton and an alpha particle have equal momentum. The ratio of their kinetic energies (EαEp) and the ratio of the de Broglie wavelengths associated with them (λαλp) respectively are : (A) 2, 1 (B) 1, 2 (C) 4, 1 (D) 1, 4
›Reveal solutionSolution
For equal momentum, kinetic energy is inversely proportional to mass, and de Broglie wavelength is directly proportional to mass. Since the alpha particle has 4 times the mass of a proton, the ratio of kinetic energies is 4:1 and the ratio of wavelengths is 1:1. The correct option is (C).
The key to this problem lies in two fundamental relationships: the de Broglie wavelength and the connection between kinetic energy and momentum. When two particles have the same momentum, their de Broglie wavelengths become equal — that part is immediate. The kinetic energy, however, depends on mass because Ek=p2/2m, so the lighter particle has more kinetic energy.
Let’s work through it systematically.
-
Recall the de Broglie wavelength formula.
Every moving particle has a wavelength associated with it, given by λ=ph, where h is Planck’s constant and p is the linear momentum. This is a direct consequence of wave-particle duality — the more momentum a particle has, the shorter its wavelength.
Since the problem states that the proton and alpha particle have equal momentum, we can write:
pp=pα
Therefore:
λp=pphandλα=pαh
Because pp=pα, the two wavelengths are identical:
λαλp=1
- Now find the kinetic energy ratio. Kinetic energy is related to momentum by:
Ek=2mp2
This comes from combining Ek=21mv2 with p=mv. For equal momentum, the kinetic energy is inversely proportional to mass — a heavier particle moving with the same momentum must be slower, so it has less kinetic energy.
For the proton (mass mp) and alpha particle (mass mα):
EαEp=p2/2mαp2/2mp=mpmα
- Know the masses involved. An alpha particle is a helium nucleus — 2 protons and 2 neutrons. Its mass is approximately 4 times the mass of a proton:
mα=4mp
This is a standard fact you should remember for such problems.
Substituting:
EαEp=mp4mp=4
- Combine the results. We have:
EαEp=4andλαλp=1
This matches option (C).
Watch outA common mistake is to forget that kinetic energy depends on mass even when momentum is fixed. Students sometimes assume Ek∝p and get the ratio wrong. Always write Ek=p2/2m explicitly.
TipFor any two particles with the same momentum, the de Broglie wavelength ratio is always 1 — it doesn’t matter what the particles are. The kinetic energy ratio is simply the inverse ratio of their masses.
✓Final answerThe correct option is (C), with EαEp=4 and λαλp=1.
-
- CBSE 2026Set V11 markMCQQ.An α-particle, a proton, an electron and a neutron are moving with the same velocity. Then the particle having longest de Broglie wavelength is :(a) proton(b) electron(c) neutron(d) α-particle
›Reveal solutionSolution
(b) electron
✓Final answer(b) electron
The de Broglie wavelength is λ=mvh. For the same velocity v, λ∝m1, so the particle with the smallest mass has the longest wavelength. Among an α-particle, proton, electron and neutron, the electron has by far the smallest mass, so it has the longest de Broglie wavelength.
- CBSE 2026Set A1 markMCQQ.The ratio of de Broglie wavelength associated with two electrons accelerated through 49 V and 64 V is (A) 49/64 (B) 64/49 (C) 7/8 (D) 8/7
›Reveal solutionSolution
de Broglie wavelength of an accelerated electron λ ∝ 1/√V; ratio = √(64/49) = 8/7.
For an electron accelerated through potential difference V, its kinetic energy is eV=2mp2, so p=2meV and the de Broglie wavelength is
λ=2meVh∝V1.
Hence
λ2λ1=V1V2=4964=78.
(The electron through the larger voltage, 64 V, has the shorter wavelength.)
✓Final answer(D) 8/7.
- CBSE 2026Set ANNUAL1 markMCQQ.If alpha particle, proton and electron move with the same momentum, then their respective de Broglie wavelengths λα, λp, λe are related as(a) λα > λp > λe(b) λα < λp < λe(c) λα = λp = λe(d) None of the above
›Reveal solutionSolution
Equal momentum means equal de Broglie wavelength, regardless of the particles' different masses.
The de Broglie wavelength of a particle is
λ=ph
where h is Planck's constant and p is the particle's momentum. This formula depends only on momentum p, not on the particle's mass, charge, or identity. Since the alpha particle, proton and electron are all stated to have the same momentum, they must all have the same de Broglie wavelength, even though their masses (and hence their speeds and kinetic energies, for the same p) are very different.
✓Final answer(c) λα=λp=λe.
- CBSE 2026Set ANNUAL1 markQ.A body of mass 0.10 kg is moving with a speed of 10 m/s. The de-Broglie wavelength of the wave associated with it will be ______ m.
›Reveal solutionSolution
The de Broglie wavelength of a moving body is lambda = h/(mv); plugging in the mass and speed gives the value directly.
De Broglie's relation: lambda = h / (m v), where h = 6.63 x 10^-34 J.s (Planck's constant), m = 0.10 kg, v = 10 m/s.
mv = 0.10 x 10 = 1 kg.m/s
lambda = 6.63 x 10^-34 / 1 = 6.63 x 10^-34 m
✓Final answerlambda = 6.63 x 10^-34 m.
- CBSE 2025Set 55/4/11 markMCQQ.Choose the correct statement: (A) Photons of light show diffraction whereas electrons do not show diffraction. (B) Electrons have momentum whereas photons do not have momentum. (C) Photons of light and electrons both exhibit dual nature. (D) All electromagnetic radiations do not have photons.
›Reveal solutionSolution
Both photons and electrons exhibit wave-particle duality — the key idea is that both show diffraction (wave behaviour) and carry momentum (particle behaviour). The correct statement is (C).
Concept First: De Broglie Wavelength and Dual Nature
The entire foundation of modern quantum mechanics rests on wave-particle duality — the idea that every moving particle has a wavelength associated with it. Louis de Broglie proposed this in 1924, and it’s summarised by:
λ=ph
where λ is the de Broglie wavelength, h is Planck’s constant, and p is the momentum.
This means:
- Photons (light quanta) have momentum p=λh and show wave phenomena like diffraction and interference.
- Electrons (particles with mass) also have a de Broglie wavelength λ=mvh and therefore do show diffraction — this was famously confirmed by Davisson and Germer in 1927.
So both photons and electrons possess both wave-like and particle-like properties. That is the dual nature.
Step-by-Step Analysis
1. Statement (A): “Photons of light show diffraction whereas electrons do not show diffraction.”
This is false. Electrons do show diffraction — the Davisson–Germer experiment proved it. In fact, electron diffraction is routinely used in techniques like transmission electron microscopy (TEM). The wavelength of an electron can be tuned by changing its accelerating voltage, making it a practical tool.
Watch outA common mistake is to think diffraction is only for light. In reality, any particle with a de Broglie wavelength comparable to the slit spacing will diffract — electrons, neutrons, even large molecules like buckyballs have been shown to diffract.
2. Statement (B): “Electrons have momentum whereas photons do not have momentum.”
This is false. Photons do have momentum, given by p=λh (or p=cE). This momentum is responsible for radiation pressure and is used in technologies like solar sails and optical tweezers. Electrons also have momentum (p=mv), but that doesn’t mean photons lack it.
3. Statement (C): “Photons of light and electrons both exhibit dual nature.”
This is true. Both show wave-like behaviour (diffraction, interference) and particle-like behaviour (momentum, discrete energy exchange). For photons, the particle aspect is evident in the photoelectric effect; for electrons, the wave aspect is seen in diffraction patterns.
4. Statement (D): “All electromagnetic radiations do not have photons.”
This is false. All electromagnetic radiation — from radio waves to gamma rays — consists of photons. The photon is the quantum of the electromagnetic field. There is no EM radiation without photons.
✓Final answerThe correct option is (C).
- CBSE 2025Set 55/5/11 markMCQQ.The kinetic energy of an alpha particle is four times the kinetic energy of a proton. The ratio λpλα of the de Broglie wavelengths associated with them will be: (A) 161 (B) 81 (C) 41 (D) 21
›Reveal solutionSolution
The de Broglie wavelength depends on momentum, not directly on kinetic energy. Using K=2mp2 and the given Kα=4Kp, along with mα=4mp, we find λpλα=41, which corresponds to option (C).
The de Broglie wavelength is the bridge between particle and wave behaviour: λ=ph, where h is Planck’s constant and p is the momentum. The problem gives you kinetic energy, not momentum directly — so the first step is always to connect K and p.
For any non-relativistic particle, kinetic energy is K=2mp2. Rearranging, p=2mK. This is the key relation that lets you translate the given energy ratio into a wavelength ratio.
-
Write the wavelength for each particle.
For the alpha particle: λα=pαh=2mαKαh.
For the proton: λp=pph=2mpKph.
-
Take the ratio.
λpλα=h/2mpKph/2mαKα=mαKαmpKp.
Notice that h and the factor 2 cancel out neatly.
-
Plug in the given data.
You are told Kα=4Kp. Also, an alpha particle is a helium nucleus — 2 protons and 2 neutrons — so its mass is approximately 4 times the proton mass: mα=4mp.
Substitute:
λpλα=(4mp)⋅(4Kp)mp⋅Kp=161=41.
Watch outA common mistake is to use λ∝1/K without accounting for mass. If you blindly write λ∝1/K, you’d get λα/λp=1/2 — which is wrong. Always include the mass factor from p=2mK.
TipYou can also think in terms of momentum directly: since Kα=4Kp and mα=4mp, we have pα=2⋅4mp⋅4Kp=32mpKp=42mpKp=4pp. So the alpha particle has 4 times the momentum of the proton, and since λ∝1/p, the wavelength ratio is 1/4.
✓Final answerThe ratio is 41, which corresponds to option (C).
-
- CBSE 2025Set X11 markMCQQ.A ball is dropped from a certain height and it falls freely under gravity. During the fall, the de Broglie wavelength associated with it :(a) keeps increasing(b) keeps decreasing(c) is zero(d) may increase or decrease
›Reveal solutionSolution
(b) keeps decreasing. The de Broglie wavelength is λ=mvh. As the ball falls freely, its speed v increases continuously, so λ (inversely proportional to v) keeps dec
✓Final answer(b) keeps decreasing.
The de Broglie wavelength is λ=mvh. As the ball falls freely, its speed v increases continuously, so λ (inversely proportional to v) keeps decreasing.
- CBSE 2025Set D1 markMCQQ.The wavelength of de Broglie wave associated with any moving particle does not depend on (A) mass (B) charge (C) velocity (D) momentum
›Reveal solutionSolution
λ = h/p = h/mv, so it depends on mass, velocity and momentum — charge does not appear in the formula.
The de Broglie wavelength of a moving particle is
λ = h/p = h/(mv)
where h is Planck's constant, m the mass, v the velocity and p = mv the momentum. The formula contains mass, velocity and momentum, so the wavelength depends on all three.
Electric charge does not appear in the expression, so the de Broglie wavelength does not depend on the charge of the particle.
✓Final answer(B) charge.
- CBSE 2025Set A1 markQ.Match Column 'A' item 'Matter waves' with the correct option from Column 'B' and write the correct pair. Column 'B' options:(i) Minimum energy to emit electrons from the surface(ii) Minimum frequency to emit electrons from the surface(iii) Frequency of photon(iv) Number of photons(v) Moving particle(vi) Photon(vii) Einstein.
›Reveal solutionSolution
Matter waves correspond to option (v): a moving particle.
Louis de Broglie proposed that, just as light exhibits both wave and particle nature, every moving material particle (electron, proton, or even a macroscopic object) has a wave associated with it, called the matter wave (or de Broglie wave), with wavelength λ=h/p, where p is the particle's momentum. This concept applies specifically to a moving particle — a particle at rest (p = 0) has an undefined (infinite) de Broglie wavelength, so 'matter waves' are intrinsically tied to a moving particle. Hence 'Matter waves' matches '(v) Moving particle'.
✓Final answerMatter waves → (v) Moving particle.
- CBSE 2025Set ANNUAL1 markMCQQ.Which of the following has the longest de-Broglie wavelength, if they are moving with same velocity ?(a) proton(b) neutron(c) α-particle(d) β-particle
›Reveal solutionSolution
At a common velocity, the lightest particle has the longest de Broglie wavelength.
The de Broglie wavelength is
λ=mvh
For a fixed velocity v (and fixed h), λ∝1/m — the smaller the mass, the longer the wavelength.
Comparing masses: proton ≈ 1836 me, neutron ≈ 1839 me, α-particle (2 protons + 2 neutrons) ≈ 4 × 1836 me, β-particle = a fast electron, mass = me (the smallest of all four by a huge margin).
✓Final answer(d) β-particle — being the least massive, it has the largest de Broglie wavelength at equal velocity.
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