How do enzymes help a substrate to be attacked by the reagent effectively?

NCERT Exemplar · Q45

Q. How do enzymes help a substrate to be attacked by the reagent effectively?

CBSEShort· 2mImportance★★★★★

71% · 78/110 Questions

🔒 Locked · start free trial →

You're viewing a preview — the full solution, concept, methods & PYQ mapping are locked.

Start your 14-day free trial to unlock the full solution →

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.

\lambda = \frac{h}{p} = \frac{h}{mv}

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:

\lambda = \frac{6.626 \times 10^{-34}}{0.16 \times 30} \approx 1.38 \times 10^{-34} \ \text{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 $9.1 \times 10^{-31}$ kg) accelerated through 100 volts. Its speed is about $5.9 \times 10^6$ m/s. Its de Broglie wavelength:

\lambda = \frac{6.626 \times 10^{-34}}{9.1 \times 10^{-31} \times 5.9 \times 10^6} \approx 1.23 \times 10^{-10} \ \text{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.

Note

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). …

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 $\lambda = \frac{h}{p}$ .

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: $p = \frac{h}{\lambda}$ (from $E = pc$ for light, combined with $c = f\lambda$ )

So for light:

\lambda = \frac{h}{p}

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 $p$ :

\boxed{\lambda = \frac{h}{p}}

Where:

$\lambda$ = de Broglie wavelength
$h$ = Planck's constant ( $6.626 \times 10^{-34} \text{ J·s}$ )
$p$ = 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):

\lambda = \frac{h}{mv}

For a relativistic particle (like an electron at high speed):

p = \gamma mv \quad \text{where} \quad \gamma = \frac{1}{\sqrt{1 - v^2/c^2}}

\lambda = \frac{h}{\gamma mv}

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: $f = \frac{E}{h}$
The wavelength comes from momentum: $\lambda = \frac{h}{p}$

These two relations are linked by the phase velocity of the wave:

v_{\text{phase}} = f\lambda = \frac{E}{h} \cdot \frac{h}{p} = \frac{E}{p}

For a free particle with kinetic energy $E = \frac{p^2}{2m}$ :

v_{\text{phase}} = \frac{p}{2m} = \frac{v}{2}

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: …

Start your 14-day free trial to unlock the full solution →

Enzymes lower the activation energy of a reaction by binding the substrate in a precise orientation and creating a local microenvironment (e.g., strain, proximity, acid-base catalysis) that makes the substrate more vulnerable to attack by a reagent. The key is transition-state stabilisation — the enzyme binds the transition state more tightly than the substrate itself.

The core idea: Why enzymes are not just passive scaffolds

A substrate in solution is surrounded by solvent molecules, jostling randomly. For a reagent to attack it, the substrate must first adopt a high-energy, unstable geometry — the transition state. In free solution, this is rare and costly. An enzyme solves this by doing three things at once:

It grabs the substrate and holds it still — reducing the entropy cost of bringing the substrate and reagent together.
It distorts the substrate — pushing it toward the transition-state geometry.
It provides chemical groups (acid, base, metal ions) that directly participate in bond breaking/forming.

Let’s walk through the mechanism step by step.

Step-by-step explanation

1. Binding in the active site — the “induced fit” lock and key

The substrate enters the enzyme’s active site, a pocket lined with specific amino acid residues. Unlike a rigid lock-and-key, most enzymes undergo induced fit: the enzyme changes shape slightly to wrap around the substrate. This does two things:

It excludes water from the reaction site, creating a low-dielectric, non-polar microenvironment. This can dramatically alter the pKa of catalytic groups and make charged intermediates more stable.
It positions the substrate so that the bond to be broken is exactly aligned with the attacking group (e.g., a nucleophile or a proton donor).

Tip

Think of the active site as a custom-made glove that not only fits the hand but also bends the fingers into the exact position needed to throw a punch.

2. Strain and distortion — pushing the substrate uphill

Many enzymes bind the substrate in a conformation that is slightly strained — closer to the transition state than to the ground state. This is called transition-state stabilisation or binding energy used for distortion.

For example, in lysozyme, the substrate (a polysaccharide) is forced into a half-chair conformation as it binds. This conformation is exactly the geometry needed for the glycosidic bond to break. The enzyme has effectively paid some of the “activation energy” cost just by binding.

K_{\text{cat}}/K_{\text{uncat}} \approx \frac{K_S}{K_{TS}}

3. Proximity and orientation — the “effective concentration” effect

By binding both the substrate and the attacking reagent (or by having the attacking group already positioned on the enzyme), the enzyme raises their effective concentration to astronomical levels.

Consider two molecules in solution at 1 mM each. Their chance of colliding with the correct orientation is tiny. In the active site, they are held within a few angstroms of each other, with the reactive atoms pointing directly at one another. This can increase the reaction rate by a factor of $10^8$ or more.

Watch out

A common mistake is to think enzymes “add energy” to the reaction. They do not — they lower the activation energy by stabilising the transition state. The overall free-energy change ( $\Delta G$ ) of the reaction is unchanged.

4. Chemical catalysis — the enzyme’s own functional groups

Enzymes carry side chains (e.g., histidine, serine, cysteine, aspartate) that act as:

Acid catalysts — donate a proton to make a leaving group better.
Base catalysts — abstract a proton to make a nucleophile stronger.
Nucleophiles — form a covalent intermediate with the substrate (e.g., serine proteases). …

Start your 14-day free trial to unlock the full solution →

Here are the common mistakes students make when explaining how enzymes facilitate effective reagent attack on a substrate, along with how to avoid each.

Mistake 1: Confusing "Lock and Key" with "Induced Fit" as the only mechanism

The Mistake: Students often state that the enzyme has a rigid, pre-shaped active site (Lock and Key) that perfectly fits the substrate, and that this fit alone is what makes the reaction happen. They forget that for most enzymes, the active site is flexible.
Why it’s wrong: The Lock and Key model explains specificity (which substrate fits), but it does not explain how the enzyme lowers activation energy to make the reagent attack effective. The Induced Fit model is more accurate here: the enzyme changes shape slightly upon substrate binding, straining bonds and creating the perfect environment for the attack.
How to avoid: Always mention Induced Fit when discussing effectiveness of attack. Say: “The enzyme’s active site is not rigid; it molds around the substrate, putting stress on specific bonds and aligning the reagent perfectly.”

Mistake 2: Forgetting the role of the active site microenvironment

The Mistake: Students think the enzyme just “holds” the substrate and reagent together, like a pair of hands. They ignore the chemical environment inside the active site.
Why it’s wrong: The active site often has acidic/basic amino acid side chains (e.g., histidine, aspartate) that act as proton donors/acceptors. This creates a local pH or charge that makes the substrate more reactive (e.g., making a carbonyl carbon more electrophilic).
How to avoid: Explicitly state: “The enzyme provides a microenvironment (e.g., low pH, high local concentration of H⁺) that stabilizes the transition state and makes the substrate more susceptible to nucleophilic attack.”

Mistake 3: Ignoring transition state stabilization

The Mistake: Students say the enzyme “binds the substrate tightly” and that’s enough. They don’t realize that the enzyme actually binds the transition state more tightly than the substrate itself.
Why it’s wrong: If the enzyme bound the substrate too tightly, it would stabilize the ground state, making the reaction harder. The key is that the active site has complementary shape and charge to the unstable, high-energy transition state, lowering the activation energy.
How to avoid: Use the phrase: “The enzyme stabilizes the transition state more than the substrate, lowering the activation energy and allowing the reagent to attack effectively.”

Mistake 4: Omitting proximity and orientation effects

The Mistake: Students focus only on chemical catalysis (e.g., acid-base) and forget the simple physical effect of bringing the reagent and substrate close together in the correct orientation.
Why it’s wrong: In solution, reagents and substrates collide randomly. The enzyme concentrates them in a small volume and holds them in the exact orientation needed for the reaction (e.g., the attacking lone pair pointing at the electrophilic center). …

Start your 14-day free trial to unlock the full solution →

Same / Similar Concept — real previous-year questions on the same or a closely similar concept, not this exact question.

Showing the 12 most recent of 70 on this concept.

CBSE 2026Set 55/1/11 markMCQ
$Q.For questions 13 to 16, two statements are given – one labelled Assertion (A) and the other labelled Reason (R). Select the correct answer from the codes (A), (B), (C) and (D) below: (A) Both Assertion (A) and Reason (R) are true and Reason (R) is the correct explanation of the Assertion (A). (B) Both Assertion (A) and Reason (R) are true, but Reason (R) is not the correct explanation of the Assertion (A). (C) Assertion (A) is true, but Reason (R) is false. (D) Both Assertion (A) and Reason (R) are false. Assertion (A) : If accelerated electrons are passed through a narrow slit, a diffraction pattern is observed. Reason (R) : Electrons behave as both particles and waves.$
›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
$\lambda = \frac{h}{p} = \frac{h}{mv}$
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.
$\theta$
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 ( $9.11 \times 10^{-31}$ kg), charge ( $-1.6 \times 10^{-19}$ 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. …
Start your 14-day free trial to see the full solution →
CBSE 2026Set 55/3/11 markMCQ
$\left(\dfrac{E_p}{E_\alpha}\right)$
›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 $E_k = p^2/2m$ , 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 $\lambda = \frac{h}{p}$ , 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:

$p_p = p_\alpha$
Therefore:
$\lambda_p = \frac{h}{p_p} \quad \text{and} \quad \lambda_\alpha = \frac{h}{p_\alpha}$
Because $p_p = p_\alpha$ , the two wavelengths are identical:
$\frac{\lambda_p}{\lambda_\alpha} = 1$

Now find the kinetic energy ratio. Kinetic energy is related to momentum by:

$E_k = \frac{p^2}{2m}$
This comes from combining $E_k = \frac12 mv^2$ 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 $m_p$ ) and alpha particle (mass $m_\alpha$ ):
$\frac{E_p}{E_\alpha} = \frac{p^2 / 2m_p}{p^2 / 2m_\alpha} = \frac{m_\alpha}{m_p}$

Know the masses involved. …
Start your 14-day free trial to see the full solution →
CBSE 2026Set V11 markMCQ
$\alpha$
(a) proton
(b) electron
(c) neutron
(d) $\alpha$ -particle
›Reveal solutionSolution

(b) electron …

Start your 14-day free trial to see the full solution →
CBSE 2026Set A1 markMCQ
$Q. The ratio of de Broglie wavelength associated with two electrons accelerated through 49 V and 64 V is (A) 49/64 (B) 64/49 (C) 7/8 (D) 8/7$
›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 $eV = \frac{p^2}{2m}$ , so $p = \sqrt{2meV}$ and the de Broglie wavelength is

$\lambda = \frac{h}{\sqrt{2meV}} \propto \frac{1}{\sqrt{V}}.$

Hence …

Start your 14-day free trial to see the full solution →
CBSE 2026Set ANNUAL1 markMCQ
$Q. If alpha particle, proton and electron move with the same momentum, then their respective de Broglie wavelengths λα, λp, λe are related as$
(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

$\lambda = \dfrac{h}{p}$

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 …

Start your 14-day free trial to see the full solution →
CBSE 2026Set ANNUAL1 mark
$Q. A body of mass 0.10 kg is moving with a speed of 10 m/s. The de-Broglie wavelength of the wave associated with it will be ______ m.$
›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. …

Start your 14-day free trial to see the full solution →
CBSE 2025Set 55/4/11 markMCQ
$Q.Choose the correct statement: (A) Photons of light show diffraction whereas electrons do not show diffraction. (B) Electrons have momentum whereas photons do not have momentum. (C) Photons of light and electrons both exhibit dual nature. (D) All electromagnetic radiations do not have photons.$
›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:
$\lambda = \frac{h}{p}$
where $\lambda$ is the de Broglie wavelength, $h$ is Planck’s constant, and $p$ is the momentum.

This means:

Photons (light quanta) have momentum $p = \frac{h}{\lambda}$ and show wave phenomena like diffraction and interference.

Electrons (particles with mass) also have a de Broglie wavelength $\lambda = \frac{h}{mv}$ 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 out

A 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.” …
Start your 14-day free trial to see the full solution →
CBSE 2025Set 55/5/11 markMCQ
$\dfrac{\lambda_{\alpha}}{\lambda_{p}}$
›Reveal solutionSolution
The de Broglie wavelength depends on momentum, not directly on kinetic energy. Using $K = \frac{p^2}{2m}$ and the given $K_\alpha = 4K_p$ , along with $m_\alpha = 4m_p$ , we find $\frac{\lambda_\alpha}{\lambda_p} = \frac{1}{4}$ , which corresponds to option (C).

The de Broglie wavelength is the bridge between particle and wave behaviour: $\lambda = \frac{h}{p}$ , 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 $K = \frac{p^2}{2m}$ . Rearranging, $p = \sqrt{2mK}$ . 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: $\lambda_\alpha = \frac{h}{p_\alpha} = \frac{h}{\sqrt{2 m_\alpha K_\alpha}}$ .

For the proton: $\lambda_p = \frac{h}{p_p} = \frac{h}{\sqrt{2 m_p K_p}}$ .

Take the ratio.

$\frac{\lambda_\alpha}{\lambda_p} = \frac{h / \sqrt{2 m_\alpha K_\alpha}}{h / \sqrt{2 m_p K_p}} = \sqrt{\frac{m_p K_p}{m_\alpha K_\alpha}}.$
Notice that $h$ and the factor $2$ cancel out neatly.

Plug in the given data.

You are told $K_\alpha = 4 K_p$ . Also, an alpha particle is a helium nucleus — 2 protons and 2 neutrons — so its mass is approximately 4 times the proton mass: $m_\alpha = 4 m_p$ .

Substitute:

$\frac{\lambda_\alpha}{\lambda_p} = \sqrt{\frac{m_p \cdot K_p}{(4 m_p) \cdot (4 K_p)}} = \sqrt{\frac{1}{16}} = \frac{1}{4}.$ …
Start your 14-day free trial to see the full solution →
CBSE 2025Set X11 markMCQ
$Q. A ball is dropped from a certain height and it falls freely under gravity. During the fall, the de Broglie wavelength associated with it :$
(a) keeps increasing
(b) keeps decreasing
(c) is zero
(d) may increase or decrease
›Reveal solutionSolution

(b) keeps decreasing. The de Broglie wavelength is $\lambda = \dfrac{h}{mv}$ . As the ball falls freely, its speed $v$ increases continuously, so $\lambda$ (inversely proportional to $v$ ) keeps dec …

Start your 14-day free trial to see the full solution →
CBSE 2025Set D1 markMCQ
$Q. The wavelength of de Broglie wave associated with any moving particle does not depend on (A) mass (B) charge (C) velocity (D) momentum$
›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.

…

Start your 14-day free trial to see the full solution →
CBSE 2025Set A1 mark
$Q. Match Column 'A' item 'Matter waves' with the correct option from Column 'B' and write the correct pair. Column 'B' options:$
(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 $\lambda = h/p$ , where p is the particle's momentum. This concept applies specifically to a moving particle — a particle at rest (p = 0) has an undef …

Start your 14-day free trial to see the full solution →
CBSE 2025Set ANNUAL1 markMCQ
$Q. Which of the following has the longest de-Broglie wavelength, if they are moving with same velocity ?$
(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

$\lambda = \frac{h}{mv}$

For a fixed velocity v (and fixed h), $\lambda \propto 1/m$ — the smaller the mass, the longer the wavelength.

…

Start your 14-day free trial to see the full solution →

←Previous questionQ44 — Which monosaccharide units are present in starch, cellulose and glycog…→Next questionQ46 — Describe the term D- and L-configuration used for amino acids with exa…

Q.How do enzymes help a substrate to be attacked by the reagent effectively?

Concept understanding — De Broglie Wavelength

De Broglie Wavelength: When Particles Start Acting Like Waves

The Core Idea

Why You Don't See It in Daily Life

What This Means Physically

Why this formula?

De Broglie Wavelength: Why the Formula Holds

The Core Insight: Nature's Symmetry

Step 1: Start with Light (What We Already Knew)

Step 2: De Broglie's Bold Hypothesis

Step 3: Why Momentum and Not Velocity?

Step 4: The Deeper Reasoning — Wave-Particle Duality

Step 5: Experimental Confirmation (Why We Believe It)

The core idea: Why enzymes are not just passive scaffolds

Step-by-step explanation

1. Binding in the active site — the “induced fit” lock and key

2. Strain and distortion — pushing the substrate uphill

3. Proximity and orientation — the “effective concentration” effect

4. Chemical catalysis — the enzyme’s own functional groups

Concept: Enzyme-Substrate Binding & Transition State Stabilisation

Method: Induced Fit Model + Transition State Stabilisation

Steps:

Mistake 1: Confusing "Lock and Key" with "Induced Fit" as the only mechanism

Mistake 2: Forgetting the role of the active site microenvironment

Mistake 3: Ignoring transition state stabilization

Mistake 4: Omitting proximity and orientation effects

Understanding Wave-Particle Duality

Examining the Assertion

Examining the Reason

Concept First: De Broglie Wavelength and Dual Nature

Step-by-Step Analysis

Q.How do enzymes help a substrate to be attacked by the reagent effectively?

The core idea: Why enzymes are not just passive scaffolds

Step-by-step explanation

1. Binding in the active site — the “induced fit” lock and key

2. Strain and distortion — pushing the substrate uphill

3. Proximity and orientation — the “effective concentration” effect

4. Chemical catalysis — the enzyme’s own functional groups

🎓Unlock everything free for 14 days

Unlock everything free for 14 days