NEET Ug . NEET Chemistry . Chemistry . Structure of Atom
Chapter 2: Structure of Atom
Ch 2
NEET Chemistry
NEET Ug
Introduction
Overview
- Dalton’s atomic theory (1808): Atom is the ultimate particle of matter.
- Explains laws: conservation of mass, constant composition, multiple proportions.
- Fails to explain electrical charging of rubbed substances (glass, ebonite).
Solved Examples
- Ex 1: Explain why Dalton’s atomic theory could not explain electrical charging of rubbed substances.
- Dalton’s theory did not consider subatomic particles or electric charge.
Practice Set
- Q1: Dalton’s atomic theory regards the atom as:
A. Divisible particle
B. Ultimate particle
C. Made of electrons
D. Electrically charged particle - Q2: Which law is NOT explained by Dalton’s atomic theory?
A. Law of conservation of mass
B. Law of constant composition
C. Law of multiple proportions
D. Electrical charging of rubbed substances - Q3: Dalton’s atomic theory was proposed in:
A. 1908
B. 1808
C. 2008
D. 1708
Answer Key
- Q1: B - Atom is considered the ultimate particle in Dalton’s theory.
- Q2: D - Dalton’s theory could not explain electrical charging phenomena.
- Q3: B - Dalton proposed the atomic theory in 1808.
Memory Aids
- Dalton’s theory = Atom is indivisible and ultimate particle.
- Fails for electrical phenomena → leads to discovery of subatomic particles.
Discovery of Sub-atomic Particles
Fundamental Particles
- Atoms consist of electrons, protons, and neutrons.
- These are called fundamental particles.
Discovery of Electron
- Discovered by J.J. Thomson using cathode ray discharge tube.
- Cathode rays: stream of negatively charged particles (electrons) from cathode to anode.
- Visible via fluorescent coating glow when rays strike it.
- Characteristics:
- Travel in straight lines without electric/magnetic field.
- Deflected by electric/magnetic fields like negatively charged particles.
- Independent of electrode material and gas type.
- Charge to mass ratio (e/m) = 1.758820 × 1011 C kg−1 (Thomson).
- Charge on electron = −1.6 × 10−19 C (Millikan oil drop experiment).
- Mass of electron = 9.1094 × 10−31 kg.
Discovery of Protons and Canal Rays
- Protons discovered by E. Goldstein using modified cathode ray tube.
- Positively charged particles depend on gas type in tube.
- Charge to mass ratio varies with gas origin.
- Some carry multiple units of fundamental charge.
- Behavior opposite to cathode rays in electric/magnetic fields.
Discovery of Neutrons
- Discovered by James Chadwick by bombarding beryllium with α-particles.
- Neutrons are neutral, mass slightly greater than protons.
Properties of Fundamental Particles
- Electron (e): charge −1, mass 9.1094 × 10−31 kg, relative charge −1.
- Proton (p): charge +1, mass ~1.6726 × 10−27 kg, relative charge +1.
- Neutron (n): charge 0, mass ~1.6749 × 10−27 kg, relative charge 0.
Solved Examples
- Ex 1: Calculate the mass of an electron given charge e = 1.6022 × 10−19 C and e/m = 1.758820 × 1011 C kg−1.
- Mass = e / (e/m) = 9.1094 × 10−31 kg.
Practice Set
- Q1: Cathode rays consist of:
A. Protons
B. Neutrons
C. Electrons
D. Alpha particles - Q2: Charge to mass ratio of electron determined by:
A. Millikan
B. Thomson
C. Chadwick
D. Goldstein - Q3: Neutrons were discovered by:
A. J.J. Thomson
B. E. Goldstein
C. James Chadwick
D. R.A. Millikan
Answer Key
- Q1: C - Cathode rays are streams of electrons.
- Q2: B - Thomson measured e/m ratio using cathode ray tube.
- Q3: C - Chadwick discovered neutrons by α-particle bombardment.
Memory Aids
- Electron: negative charge, discovered by Thomson.
- Proton: positive charge, discovered by Goldstein.
- Neutron: neutral, discovered by Chadwick.
- Charge to mass ratio (e/m) key for electron identification.
Atomic Models
Evolution of Atomic Models
- Dalton (1808): Atoms of each element are unique and indivisible.
- Thomson (1898): Atom is a positive sphere with embedded electrons (raisin pudding model).
- Rutherford (1911): Atom has a small, dense, positively charged nucleus; most of atom is empty space.
- Bohr (1913): Electrons move in fixed orbits around nucleus; explained atomic spectra.
- Schrödinger (1926): Electrons form a cloud; exact position uncertain; wave equation predicts electron probability.
Solved Examples
- Ex 1: Identify the model describing electrons as embedded in a positive sphere.
Answer: Thomson's raisin pudding model. - Ex 2: Which model introduced the concept of a nucleus?
Answer: Rutherford's nuclear model.
Practice Set
- Q1: Who proposed the electron cloud model?
A. Dalton
B. Thomson
C. Schrödinger
D. Bohr - Q2: Rutherford's experiment showed that most of the atom is:
A. Solid
B. Empty space
C. Uniformly positive
D. Negatively charged - Q3: Which model explains the stability of atom by fixed electron orbits?
A. Dalton
B. Thomson
C. Bohr
D. Schrödinger
Answer Key
- Q1: C - Schrödinger proposed the electron cloud model where electron position is probabilistic.
- Q2: B - Rutherford's scattering showed most alpha particles passed through, indicating empty space.
- Q3: C - Bohr's model introduced fixed orbits explaining atomic stability and spectra.
Memory Aids
- Dalton: "Distinct atoms"
- Thomson: "Raisin pudding" = electrons in positive sphere
- Rutherford: "Nucleus discovery"
- Bohr: "Fixed orbits"
- Schrödinger: "Electron cloud"
Thomson Model
Key Features
- Atom is a sphere of uniformly distributed positive charge.
- Electrons (negative charges) are embedded like raisins in pudding.
- Mass is uniformly distributed over the atom.
- Explains overall electrical neutrality of atom.
- Fails to explain later experimental results.
Solved Examples
- Ex 1: Describe the charge distribution in Thomson's model.
Answer: Positive charge uniformly spread; electrons embedded within.
Practice Set
- Q1: Thomson's model compares electrons to:
A. Planets
B. Raisins in pudding
C. Orbiting satellites
D. Nucleus - Q2: What is assumed about the mass distribution in Thomson's model?
A. Concentrated in nucleus
B. Uniformly distributed
C. Only in electrons
D. Only in positive sphere - Q3: Thomson's model fails to explain:
A. Atom's neutrality
B. Electron discovery
C. Later experimental results
D. Presence of nucleus
Answer Key
- Q1: B - Electrons are like raisins embedded in positive pudding.
- Q2: B - Mass is assumed uniformly distributed over the atom.
- Q3: C - Model inconsistent with later experiments like Rutherford's.
Memory Aids
- "Raisin pudding" = electrons in positive sphere
- Mass uniform, no nucleus concept
Rutherford Model
Key Observations
- Alpha particles mostly pass through gold foil undeflected → atom mostly empty space.
- Some alpha particles deflected at small and large angles → presence of small, dense, positively charged nucleus.
- Few alpha particles reflected back → nucleus is hard and dense.
- Nucleus radius ~10-15 m; atom radius ~10-10 m.
- Electrons revolve around nucleus in circular orbits.
- Electrostatic attraction holds electrons and nucleus together.
- Penetrating power: γ-rays > X-rays > β-rays > α-rays.
- Atomic number (Z) = number of protons = number of electrons in neutral atom.
- Mass number (A) = protons + neutrons.
Solved Examples
- Ex 1: What conclusion was drawn from most alpha particles passing through gold foil?
Answer: Atom is mostly empty space. - Ex 2: Define atomic number.
Answer: Number of protons in nucleus = number of electrons in neutral atom.
Practice Set
- Q1: What does Rutherford's experiment prove about atom?
A. Solid sphere
B. Mostly empty space
C. Uniform positive charge
D. No nucleus - Q2: Atomic number represents:
A. Number of neutrons
B. Number of protons
C. Number of electrons only
D. Mass number - Q3: Which ray has the highest penetrating power?
A. α-rays
B. β-rays
C. X-rays
D. γ-rays
Answer Key
- Q1: B - Most alpha particles passed through, showing atom is mostly empty space.
- Q2: B - Atomic number is number of protons in nucleus.
- Q3: D - γ-rays have highest penetrating power.
Memory Aids
- "Gold foil experiment" → nucleus discovery
- Penetrating power order: γ > X > β > α
- Atomic number = protons = electrons (neutral atom)
Drawbacks of Rutherford Model
Limitations
- Electrons revolving in orbits should emit radiation and lose energy → atom collapse (not observed).
- Calculated collapse time ~10-8 s, but atoms are stable.
- No explanation of electron energy levels or distribution.
Solved Examples
- Ex 1: Why is Rutherford's model unable to explain atomic stability?
Answer: Accelerating electrons should emit radiation and spiral into nucleus.
Practice Set
- Q1: According to Rutherford, electrons in orbits should:
A. Remain stable
B. Emit radiation and lose energy
C. Not move
D. Gain energy - Q2: Rutherford's model fails to explain:
A. Nucleus existence
B. Electron energy levels
C. Atomic number
D. Alpha particle scattering - Q3: Time for electron to spiral into nucleus is approximately:
A. 108 s
B. 10-8 s
C. 1 s
D. Infinite
Answer Key
- Q1: B - Accelerating electrons should emit radiation and lose energy.
- Q2: B - Model does not explain electron energy levels or distribution.
- Q3: B - Calculated collapse time is about 10-8 seconds.
Memory Aids
- "Electron radiation loss" → instability in Rutherford model
- Need for Bohr model to explain stability
Developments Leading to Bohr's Model
Wave Nature of Electromagnetic Radiations
- Energy emitted continuously as electromagnetic waves with perpendicular electric and magnetic fields.
- Electric and magnetic fields vibrate in mutually perpendicular planes.
- Wave travels in one direction with electric and magnetic fields oscillating perpendicular to it.
Characteristic Properties of Electromagnetic Waves
- Frequency (ν): Number of waves passing a point per second (Hz or s-1).
- Wavelength (λ): Distance between two consecutive crests or troughs (m, Å, pm, nm).
- Velocity (c): Speed of wave in vacuum = 3.0 × 108 m/s; c = νλ.
- Wavenumber (ν̅): Number of wavelengths per unit length (m-1, commonly cm-1).
- Amplitude: Height of crest or depth of trough; determines light intensity.
- Relations: c = νλ, ν = c/λ, ν̅ = 1/λ.
Electromagnetic Spectrum
- Arrangement of electromagnetic radiations by increasing wavelength or decreasing frequency.
- Includes gamma rays, X-rays, UV, visible light, infrared, microwaves, and radio waves.
- Visible spectrum ranges from violet (short wavelength) to red (long wavelength).
Black Body Radiation and Planck's Quantum Theory
- Black body: Ideal body absorbing and emitting all frequencies.
- Planck's theory: Energy emitted/absorbed in discrete packets called quanta.
- Energy of quantum: E = hν, where h = 6.626 × 10-34 J·s.
- Total energy: E = nhν, n = integer (0,1,2,...).
Photoelectric Effect
- Emission of electrons from metal surface when light of minimum frequency (threshold frequency ν0) shines on it.
- Light consists of photons transferring energy to electrons.
- Electrons ejected are called photoelectrons.
- Kinetic energy of ejected electron: hν = hν0 + 1/2 mev2.
- Work function (hν0): Minimum energy to eject electron.
- Demonstrates particle nature of light.
Dual Nature of Electromagnetic Radiation
- Light behaves as wave during propagation and as particles during interaction with matter.
Spectrum Types
- Combination of lights of different wavelengths analyzed through a prism.
- Atomic spectra: line, band, continuous.
- Molecular spectra: absorption, emission, discontinuous.
Hydrogen Atomic Spectra
- Spectral lines grouped into series: Lyman (UV), Balmer (visible), Paschen, Brackett, Pfund (infrared).
- Electron transitions between energy levels n1 and n2 produce these lines.
- Maximum number of lines from n to 1: n(n–1)/2.
- Lines from n2 to n1: (n2 – n1)(n2 – n1 + 1)/2.
Solved Examples
- Ex 1: Calculate wavelength if frequency is 6 × 1014 Hz.
Solution: λ = c/ν = (3 × 108 m/s) / (6 × 1014 Hz) = 5 × 10-7 m (visible light). - Ex 2: Find kinetic energy of photoelectron if hν = 5 eV and work function hν0 = 2 eV.
Solution: KE = hν - hν0 = 5 - 2 = 3 eV. - Ex 3: Number of spectral lines when electron falls from n=4 to n=1.
Solution: n(n-1)/2 = 4×3/2 = 6 lines.
Practice Set
- Q1: What is the speed of electromagnetic waves in vacuum?
A. 3 × 106 m/s
B. 3 × 108 m/s
C. 3 × 1010 m/s
D. 3 × 105 m/s - Q2: Which series of hydrogen spectrum lies in the visible region?
A. Lyman
B. Balmer
C. Paschen
D. Brackett - Q3: Calculate the wavelength of light if frequency is 5 × 1014 Hz.
A. 6 × 10-7 m
B. 5 × 10-7 m
C. 4 × 10-7 m
D. 3 × 10-7 m
Answer Key
- Q1: B. 3 × 108 m/s - Speed of light in vacuum.
- Q2: B. Balmer - Visible region series of hydrogen.
- Q3: B. 5 × 10-7 m - Using λ = c/ν.
Memory Aids
- Speed of light c = 3 × 108 m/s.
- Energy quantum E = hν; Planck's constant h = 6.626 × 10-34 J·s.
- Visible spectrum: VIBGYOR (Violet shortest λ, Red longest λ).
- Photoelectric effect metals: K, Rb, Cs.
- Max spectral lines from n: n(n-1)/2.
Bohr's Model for Hydrogen Atom
Key Concepts
- Electrons move in fixed circular orbits (energy shells) around the nucleus with fixed radius and energy.
- Energy of an electron in a given orbit remains constant over time.
- Electron absorbs energy to jump to a higher orbit and releases energy when falling back to a lower orbit.
- Energy levels follow: E1 < E2 < E3 ...
- Energy difference between levels: ΔE = E2 – E1 = hν, with ΔE decreasing for higher orbits.
- Angular momentum quantization: mvr = nh/2π, where n = 1, 2, 3...
- Energy of nth orbit: En = –RH (Z2/n2) = –2.18×10–18 × Z2/n2 J.
- Rydberg constant RH = 2.18 × 10–18 J.
- Radius of nth orbit for hydrogen: rn = 0.529 × n2 Å.
- For one-electron species with atomic number Z: rn = 0.529 × n2/Z Å.
Solved Examples
- Ex 1: Calculate the radius of the 3rd orbit of hydrogen.
- Use rn = 0.529 × n2 Å
- r3 = 0.529 × 32 = 0.529 × 9 = 4.761 Å
- Ex 2: Find the energy of the 2nd orbit of He+ (Z=2).
- En = –2.18×10–18 × Z2/n2 J
- E2 = –2.18×10–18 × 4/4 = –2.18×10–18 J
Practice Set
- Q1: What is the angular momentum of an electron in the 1st orbit?
- A. 0
- B. h/2π
- C. 2h/2π
- D. nh
- Q2: The radius of the 4th orbit of hydrogen atom is:
- A. 0.529 Å
- B. 8.464 Å
- C. 0.529 × 16 Å
- D. 2.116 Å
- Q3: Energy difference between 2nd and 1st orbit is:
- A. hν
- B. E2 – E1
- C. Both A and B
- D. None
Answer Key
- Q1: B - Angular momentum is quantized as mvr = nh/2π, for n=1 it is h/2π.
- Q2: C - r4 = 0.529 × 42 = 0.529 × 16 Å.
- Q3: C - Energy difference ΔE = E2 – E1 = hν.
Memory Aids
- Angular momentum quantization: "n times h over 2 pi".
- Radius scales as n squared: "Radius ∝ n2".
- Energy levels are negative and inversely proportional to n squared.
Rydberg Formula
Key Concepts
- Used for hydrogen and hydrogen-like atoms to calculate spectral lines.
- Formula: 1/λ = ν = R [1/n12 – 1/n22] Z2
- R = 109,677 cm–1 (Rydberg constant in wave numbers).
- Z is the atomic number.
Solved Examples
- Ex 1: Calculate wavelength for transition n2=3 to n1=2 in hydrogen (Z=1).
- 1/λ = R [1/22 – 1/32] = 109,677 [1/4 – 1/9]
- 1/λ = 109,677 × (5/36) = 15,243 cm–1
- λ = 1/15,243 cm = 6.56 × 10–5 cm = 656 nm
Practice Set
- Q1: What is the value of Rydberg constant R?
- A. 109,677 cm–1
- B. 2.18 × 10–18 J
- C. 0.529 Å
- D. 6.626 × 10–34 Js
- Q2: For hydrogen, the spectral line corresponds to transition from n=4 to n=2. Which formula is used?
- A. En = –RH Z2/n2
- B. 1/λ = R [1/n12 – 1/n22] Z2
- C. mvr = nh/2π
- D. rn = 0.529 n2/Z
- Q3: What does Z represent in the Rydberg formula?
- A. Principal quantum number
- B. Atomic number
- C. Energy level
- D. Wavelength
Answer Key
- Q1: A - Rydberg constant R = 109,677 cm–1.
- Q2: B - Rydberg formula calculates spectral lines for transitions.
- Q3: B - Z is the atomic number.
Memory Aids
- Rydberg formula relates inverse wavelength to energy level differences.
- Remember R = 109,677 cm–1 for hydrogen.
- Z squared factor accounts for nuclear charge effect.
Limitations of Bohr's Theory
Key Points
- Fails to explain spectra of multi-electron atoms.
- Cannot explain electron distribution in atoms.
- Does not account for splitting of spectral lines under magnetic (Zeeman effect) and electric fields (Stark effect).
- Ignores wave-particle duality and Heisenberg's uncertainty principle.
Solved Examples
- Ex 1: Why can't Bohr's model explain Zeeman effect?
- Because it ignores electron spin and magnetic interactions.
Practice Set
- Q1: Which phenomenon is NOT explained by Bohr's model?
- A. Hydrogen spectrum
- B. Zeeman effect
- C. Energy quantization
- D. Radius of orbits
- Q2: Bohr's model ignores which principle?
- A. Conservation of energy
- B. Uncertainty principle
- C. Pauli exclusion principle
- D. Aufbau principle
- Q3: Bohr's model is limited to atoms with how many electrons?
- A. One
- B. Two
- C. Many
- D. Zero
Answer Key
- Q1: B - Zeeman effect involves magnetic splitting not explained by Bohr's model.
- Q2: B - It ignores the uncertainty principle.
- Q3: A - Applicable only to one-electron atoms/ions.
Memory Aids
- Bohr's model = "One electron only" model.
- Does not explain magnetic/electric field effects on spectra.
- Ignores wave nature and uncertainty principle.
Towards Quantum Mechanical Model of the Atom
Wave-particle duality and de Broglie’s equation
- Electrons exhibit dual nature: particle and wave.
- de Broglie equation: λ = h/p = h/mv, where λ is wavelength, h Planck's constant, p momentum.
- Relation: E = mc2 = hν = hc/λ.
- Every moving object has wave character; de Broglie waves are associated with electrons only.
- Wavelength decreases with increasing mass; negligible for heavy particles.
- Applicable mainly to subatomic particles like electrons.
- Alternate form: λ = h/√(2mEk) = h/√(2mqV), where Ek kinetic energy, q charge, m mass, V accelerating potential.
Solved Examples
- Ex 1: Calculate wavelength of electron accelerated through 100 V.
- Use λ = h/√(2mqV).
- Substitute values: h = 6.626 × 10-34 Js, m = 9.11 × 10-31 kg, q = 1.6 × 10-19 C, V = 100 V.
- Calculate λ in meters.
Practice Set
- Q1: What is the de Broglie wavelength of a particle with momentum 2 × 10-24 kg , m/s?
- A) 3.3 × 10-10 m
- B) 6.6 × 10-34 m
- C) 1.0 × 10-10 m
- D) 1.2 × 10-9 m
- Q2: Which particle has the largest de Broglie wavelength?
- A) Electron
- B) Proton
- C) Neutron
- D) Alpha particle
- Q3: The wavelength of a particle is inversely proportional to:
- A) Mass
- B) Velocity
- C) Momentum
- D) All of the above
Answer Key
- Q1: A - λ = h/p = 6.626 × 10-34/(2 × 10-24) = 3.3 × 10-10 m.
- Q2: A - Electron has smallest mass, hence largest wavelength.
- Q3: C - Wavelength inversely proportional to momentum p = mv.
Memory Aids
- de Broglie wavelength λ = h/mv remember as "wavelength inversely proportional to momentum".
- Wave nature significant only for very small mass particles.
- Heavier particles have negligible wave properties.
Wave-particle duality and de Broglie’s equation
- Electrons exhibit dual nature: particle and wave.
- de Broglie equation: \( \lambda = \frac{h}{p} = \frac{h}{mv} \), where \( \lambda \) is wavelength, \( h \) Planck's constant, \( p \) momentum.
- Relation: \( E = mc^2 = h\nu = \frac{hc}{\lambda} \).
- Every moving object has wave character; de Broglie waves are associated with electrons only.
- Wavelength decreases with increasing mass; negligible for heavy particles.
- Applicable mainly to subatomic particles like electrons.
- Alternate form: \( \lambda = \frac{h}{\sqrt{2mE_k}} = \frac{h}{\sqrt{2mqV}} \), where \( E_k \) kinetic energy, \( q \) charge, \( m \) mass, \( V \) accelerating potential.
Solved Examples
- Ex 1: Calculate wavelength of electron accelerated through 100 V.
- Use \( \lambda = \frac{h}{\sqrt{2mqV}} \).
- Substitute values: \( h = 6.626 \times 10^{-34} Js \), \( m = 9.11 \times 10^{-31} kg \), \( q = 1.6 \times 10^{-19} C \), \( V = 100 V \).
- Calculate \( \lambda \) in meters.
Practice Set
- Q1: What is the de Broglie wavelength of a particle with momentum \( 2 \times 10^{-24} kg \, m/s \)?
- A) \( 3.3 \times 10^{-10} m \)
- B) \( 6.6 \times 10^{-34} m \)
- C) \( 1.0 \times 10^{-10} m \)
- D) \( 1.2 \times 10^{-9} m \)
- Q2: Which particle has the largest de Broglie wavelength?
- A) Electron
- B) Proton
- C) Neutron
- D) Alpha particle
- Q3: The wavelength of a particle is inversely proportional to:
- A) Mass
- B) Velocity
- C) Momentum
- D) All of the above
Answer Key
- Q1: A - \( \lambda = \frac{h}{p} = \frac{6.626 \times 10^{-34}}{2 \times 10^{-24}} = 3.3 \times 10^{-10} m \).
- Q2: A - Electron has smallest mass, hence largest wavelength.
- Q3: C - Wavelength inversely proportional to momentum \( p = mv \).
Memory Aids
- de Broglie wavelength \( \lambda = \frac{h}{mv} \) remember as "wavelength inversely proportional to momentum".
- Wave nature significant only for very small mass particles.
- Heavier particles have negligible wave properties.
Heisenberg’s Uncertainty Principle
Principle and significance
- It is impossible to simultaneously know exact position (Δx) and momentum (Δp) of an electron.
- Mathematically: Δx × Δp ≥ h/4π or Δx × mΔv ≥ h/4π.
- Uncertainty principle rules out definite electron paths or trajectories.
- Significant only for microscopic particles; negligible for macroscopic objects.
Solved Examples
- Ex 1: Calculate minimum uncertainty in position if uncertainty in momentum is 1 × 10-24 kg , m/s.
- Use Δx ≥ h/(4πΔp).
- Substitute h = 6.626 × 10-34 Js, Δp = 1 × 10-24 kg , m/s.
- Calculate Δx in meters.
Practice Set
- Q1: Heisenberg’s uncertainty principle states that:
- A) Position and momentum can be known exactly.
- B) Position and momentum cannot be known simultaneously with exact precision.
- C) Only position can be known exactly.
- D) Only momentum can be known exactly.
- Q2: If uncertainty in position decreases, uncertainty in momentum:
- A) Decreases
- B) Increases
- C) Remains same
- D) Becomes zero
- Q3: The uncertainty principle is most significant for:
- A) Macroscopic objects
- B) Microscopic particles
- C) Both equally
- D) None
Answer Key
- Q1: B - Exact simultaneous knowledge of position and momentum is impossible.
- Q2: B - Decreasing uncertainty in position increases uncertainty in momentum.
- Q3: B - Principle applies mainly to microscopic particles like electrons.
Memory Aids
- Remember: Δx × Δp ≥ h/4π means position and momentum cannot both be exact.
- Uncertainty principle forbids exact electron paths.
- Significant only at atomic/subatomic scale.
Principle and significance
- It is impossible to simultaneously know exact position (\( \Delta x \)) and momentum (\( \Delta p \)) of an electron.
- Mathematically: \( \Delta x \times \Delta p \geq \frac{h}{4\pi} \) or \( \Delta x \times m \Delta v \geq \frac{h}{4\pi} \).
- Uncertainty principle rules out definite electron paths or trajectories.
- Significant only for microscopic particles; negligible for macroscopic objects.
Solved Examples
- Ex 1: Calculate minimum uncertainty in position if uncertainty in momentum is \( 1 \times 10^{-24} kg \, m/s \).
- Use \( \Delta x \geq \frac{h}{4\pi \Delta p} \).
- Substitute \( h = 6.626 \times 10^{-34} Js \), \( \Delta p = 1 \times 10^{-24} kg \, m/s \).
- Calculate \( \Delta x \) in meters.
Practice Set
- Q1: Heisenberg’s uncertainty principle states that:
- A) Position and momentum can be known exactly.
- B) Position and momentum cannot be known simultaneously with exact precision.
- C) Only position can be known exactly.
- D) Only momentum can be known exactly.
- Q2: If uncertainty in position decreases, uncertainty in momentum:
- A) Decreases
- B) Increases
- C) Remains same
- D) Becomes zero
- Q3: The uncertainty principle is most significant for:
- A) Macroscopic objects
- B) Microscopic particles
- C) Both equally
- D) None
Answer Key
- Q1: B - Exact simultaneous knowledge of position and momentum is impossible.
- Q2: B - Decreasing uncertainty in position increases uncertainty in momentum.
- Q3: B - Principle applies mainly to microscopic particles like electrons.
Memory Aids
- Remember: \( \Delta x \times \Delta p \geq \frac{h}{4\pi} \) means position and momentum cannot both be exact.
- Uncertainty principle forbids exact electron paths.
- Significant only at atomic/subatomic scale.
Quantum Mechanical Model of Atom
Key Concepts
- Schrodinger wave equation: ∂2ψ/∂x2 + ∂2ψ/∂y2 + ∂2ψ/∂z2 + 8π2m/h2 (E - V) ψ = 0
- ψ is the wave function; ψ2 gives the probability density of finding an electron in a small region.
- Atomic orbital: 3D space around nucleus with maximum electron probability.
- Energy of electrons is quantized due to wave nature and solutions of Schrodinger equation.
- Exact position and velocity of electron cannot be known simultaneously (Heisenberg uncertainty principle).
- Probability density ψ2 is always positive and proportional to electron presence.
Solved Examples
- Ex 1: Write the Schrodinger wave equation for an electron in an atom.
Answer: ∂2ψ/∂x2 + ∂2ψ/∂y2 + ∂2ψ/∂z2 + 8π2m/h2 (E - V) ψ = 0
Practice Set
- Q1: What does ψ2 represent in the quantum mechanical model?
A. Electron velocity
B. Electron position
C. Probability density of electron
D. Energy of electron - Q2: Which principle states that exact position and velocity of electron cannot be known simultaneously?
A. Pauli exclusion principle
B. Hund’s rule
C. Heisenberg uncertainty principle
D. Aufbau principle - Q3: An atomic orbital is defined as:
A. A point where electron is found
B. A 2D space around nucleus
C. A 3D space with maximum electron probability
D. The path of electron around nucleus
Answer Key
- Q1: C - ψ2 gives the probability density of finding an electron.
- Q2: C - Heisenberg uncertainty principle limits simultaneous knowledge of position and velocity.
- Q3: C - Atomic orbital is a 3D region with maximum probability of electron presence.
Memory Aids
- Remember: ψ is wave function, ψ2 is probability density.
- Heisenberg uncertainty = no exact position & velocity simultaneously.
- Atomic orbital = 3D region of max electron probability.
Key Concepts
- Schrodinger wave equation: \( \frac{\partial^2 \psi}{\partial x^2} + \frac{\partial^2 \psi}{\partial y^2} + \frac{\partial^2 \psi}{\partial z^2} + \frac{8 \pi^2 m}{h^2} (E - V) \psi = 0 \)
- \( \psi \) is the wave function; \( \psi^2 \) gives the probability density of finding an electron in a small region.
- Atomic orbital: 3D space around nucleus with maximum electron probability.
- Energy of electrons is quantized due to wave nature and solutions of Schrodinger equation.
- Exact position and velocity of electron cannot be known simultaneously (Heisenberg uncertainty principle).
- Probability density \( \psi^2 \) is always positive and proportional to electron presence.
Solved Examples
- Ex 1: Write the Schrodinger wave equation for an electron in an atom.
Answer: \( \frac{\partial^2 \psi}{\partial x^2} + \frac{\partial^2 \psi}{\partial y^2} + \frac{\partial^2 \psi}{\partial z^2} + \frac{8 \pi^2 m}{h^2} (E - V) \psi = 0 \)
Practice Set
- Q1: What does \( \psi^2 \) represent in the quantum mechanical model?
A. Electron velocity
B. Electron position
C. Probability density of electron
D. Energy of electron - Q2: Which principle states that exact position and velocity of electron cannot be known simultaneously?
A. Pauli exclusion principle
B. Hund’s rule
C. Heisenberg uncertainty principle
D. Aufbau principle - Q3: An atomic orbital is defined as:
A. A point where electron is found
B. A 2D space around nucleus
C. A 3D space with maximum electron probability
D. The path of electron around nucleus
Answer Key
- Q1: C - \( \psi^2 \) gives the probability density of finding an electron.
- Q2: C - Heisenberg uncertainty principle limits simultaneous knowledge of position and velocity.
- Q3: C - Atomic orbital is a 3D region with maximum probability of electron presence.
Memory Aids
- Remember: \( \psi \) is wave function, \( \psi^2 \) is probability density.
- Heisenberg uncertainty = no exact position & velocity simultaneously.
- Atomic orbital = 3D region of max electron probability.
Quantum Numbers
Key Concepts
- Four quantum numbers describe an electron completely: Principal (n), Azimuthal (l), Magnetic (ml), Spin (ms).
- Principal quantum number (n): Energy level/shell (1, 2, 3, ...).
- Azimuthal quantum number (l): Subshell shape (0 to n-1), s=0, p=1, d=2, f=3.
- Magnetic quantum number (ml): Orbital orientation (-l to +l).
- Spin quantum number (ms): Electron spin (+1/2 or -1/2).
- Number of subshells in nth shell = n; orbitals = n2; max electrons = 2n2.
- Orbitals in subshell = 2l + 1; max electrons = 2(2l + 1).
Solved Examples
- Ex 1: Find the number of orbitals in the 3rd shell.
Solution: Number of orbitals = n2 = 32 = 9. - Ex 2: What is the range of ml for l = 2?
Solution: ml = -2, -1, 0, +1, +2.
Practice Set
- Q1: What is the maximum number of electrons in the 2nd shell?
A. 2
B. 8
C. 18
D. 32 - Q2: The azimuthal quantum number for p-orbital is:
A. 0
B. 1
C. 2
D. 3 - Q3: How many orbitals are there in the d-subshell?
A. 3
B. 5
C. 7
D. 9
Answer Key
- Q1: B - Max electrons = 2n2 = 2(2)2 = 8.
- Q2: B - p-orbital corresponds to l = 1.
- Q3: B - Number of orbitals in d-subshell = 2l + 1 = 5.
Memory Aids
- n = shell number; l = subshell shape (s=0, p=1, d=2, f=3).
- ml ranges from -l to +l.
- ms = +1/2 or -1/2 (spin up/down).
Key Concepts
- Four quantum numbers describe an electron completely: Principal (n), Azimuthal (l), Magnetic (ml), Spin (ms).
- Principal quantum number (n): Energy level/shell (1, 2, 3, ...).
- Azimuthal quantum number (l): Subshell shape (0 to n-1), s=0, p=1, d=2, f=3.
- Magnetic quantum number (ml): Orbital orientation (-l to +l).
- Spin quantum number (ms): Electron spin (+1/2 or -1/2).
- Number of subshells in nth shell = n; orbitals = n2; max electrons = 2n2.
- Orbitals in subshell = 2l + 1; max electrons = 2(2l + 1).
Solved Examples
- Ex 1: Find the number of orbitals in the 3rd shell.
Solution: Number of orbitals = n2 = 32 = 9. - Ex 2: What is the range of ml for l = 2?
Solution: ml = -2, -1, 0, +1, +2.
Practice Set
- Q1: What is the maximum number of electrons in the 2nd shell?
A. 2
B. 8
C. 18
D. 32 - Q2: The azimuthal quantum number for p-orbital is:
A. 0
B. 1
C. 2
D. 3 - Q3: How many orbitals are there in the d-subshell?
A. 3
B. 5
C. 7
D. 9
Answer Key
- Q1: B - Max electrons = 2n2 = 2(2)2 = 8.
- Q2: B - p-orbital corresponds to l = 1.
- Q3: B - Number of orbitals in d-subshell = 2l + 1 = 5.
Memory Aids
- n = shell number; l = subshell shape (s=0, p=1, d=2, f=3).
- ml ranges from -l to +l.
- ms = +1/2 or -1/2 (spin up/down).
Shapes of Atomic Orbitals
Key Concepts
- Orbital shape given by total probability density ψ2 (radial + angular parts).
- 1s orbital: spherical shape, max probability at nucleus, decreases outward.
- 2s orbital: has radial node where probability density is zero.
- Nodes: regions where probability density is zero; radial nodes = n - l - 1, angular nodes = l, total nodes = n - 1.
- p-orbitals: dumbbell shape with two lobes along x, y, z axes; one nodal plane through nucleus.
- d-orbitals: clover-leaf shape; five types; dz2 has doughnut shape; two nodal planes each.
Solved Examples
- Ex 1: Calculate radial nodes for 3p orbital.
Solution: Radial nodes = n - l - 1 = 3 - 1 - 1 = 1. - Ex 2: Describe shape of p-orbital.
Solution: Dumbbell shape with two lobes opposite nucleus along an axis.
Practice Set
- Q1: Number of total nodes in 4d orbital?
A. 2
B. 3
C. 4
D. 5 - Q2: Shape of s-orbital is:
A. Dumbbell
B. Spherical
C. Clover-leaf
D. Doughnut - Q3: How many nodal planes does a d-orbital have?
A. 1
B. 2
C. 3
D. 4
Answer Key
- Q1: C - Total nodes = n - 1 = 4 - 1 = 3.
- Q2: B - s-orbitals are spherical.
- Q3: B - Each d-orbital has two nodal planes.
Memory Aids
- s = spherical, p = dumbbell, d = clover-leaf.
- Nodes total = n - 1; radial = n - l - 1; angular = l.
- dz2 orbital has doughnut shape.
Key Concepts
- Orbital shape given by total probability density \( \psi^2 \) (radial + angular parts).
- 1s orbital: spherical shape, max probability at nucleus, decreases outward.
- 2s orbital: has radial node where probability density is zero.
- Nodes: regions where probability density is zero; radial nodes = n - l - 1, angular nodes = l, total nodes = n - 1.
- p-orbitals: dumbbell shape with two lobes along x, y, z axes; one nodal plane through nucleus.
- d-orbitals: clover-leaf shape; five types; dz^2 has doughnut shape; two nodal planes each.
Solved Examples
- Ex 1: Calculate radial nodes for 3p orbital.
Solution: Radial nodes = n - l - 1 = 3 - 1 - 1 = 1. - Ex 2: Describe shape of p-orbital.
Solution: Dumbbell shape with two lobes opposite nucleus along an axis.
Practice Set
- Q1: Number of total nodes in 4d orbital?
A. 2
B. 3
C. 4
D. 5 - Q2: Shape of s-orbital is:
A. Dumbbell
B. Spherical
C. Clover-leaf
D. Doughnut - Q3: How many nodal planes does a d-orbital have?
A. 1
B. 2
C. 3
D. 4
Answer Key
- Q1: C - Total nodes = n - 1 = 4 - 1 = 3.
- Q2: B - s-orbitals are spherical.
- Q3: B - Each d-orbital has two nodal planes.
Memory Aids
- s = spherical, p = dumbbell, d = clover-leaf.
- Nodes total = n - 1; radial = n - l - 1; angular = l.
- dz^2 orbital has doughnut shape.
Energy of Orbitals
Key Concepts
- In hydrogen atom, energy depends only on principal quantum number (n).
- Energy order: 1s < 2s < 2p < 3s < 3p < 4s < 3d < 4p < 5s < 4d < 5p < 6s < 4f < ...
- Orbitals with same energy are degenerate.
- 1s orbital is ground state; higher orbitals are excited states.
- In multi-electron atoms, energy depends on n and l.
- Lower (n + l) means lower energy; if equal, lower n means lower energy.
- Energy decreases with increasing atomic number (Zeff) in same subshell.
Solved Examples
- Ex 1: Arrange orbitals in increasing energy for hydrogen: 3p, 2s, 1s.
Answer: 1s < 2s < 3p. - Ex 2: Which orbital has lower energy: 4s or 3d?
Answer: 4s has lower energy than 3d.
Practice Set
- Q1: Which orbital is degenerate with 2p in hydrogen atom?
A. 2s
B. 3s
C. 1s
D. 3p - Q2: In multi-electron atoms, energy depends on:
A. Only n
B. Only l
C. Both n and l
D. Neither n nor l - Q3: Which has the lowest energy?
A. 3d
B. 4s
C. 4p
D. 3p
Answer Key
- Q1: A - 2s and 2p are degenerate in hydrogen.
- Q2: C - Energy depends on both n and l in multi-electron atoms.
- Q3: B - 4s has lower energy than 3d and 4p.
Memory Aids
- Energy order follows (n + l) rule.
- Degenerate orbitals have same energy in hydrogen.
- 4s fills before 3d due to lower energy.
Key Concepts
- In hydrogen atom, energy depends only on principal quantum number (n).
- Energy order: 1s < 2s < 2p < 3s < 3p < 4s < 3d < 4p < 5s < 4d < 5p < 6s < 4f < ...
- Orbitals with same energy are degenerate.
- 1s orbital is ground state; higher orbitals are excited states.
- In multi-electron atoms, energy depends on n and l.
- Lower (n + l) means lower energy; if equal, lower n means lower energy.
- Energy decreases with increasing atomic number (Zeff) in same subshell.
Solved Examples
- Ex 1: Arrange orbitals in increasing energy for hydrogen: 3p, 2s, 1s.
Answer: 1s < 2s < 3p. - Ex 2: Which orbital has lower energy: 4s or 3d?
Answer: 4s has lower energy than 3d.
Practice Set
- Q1: Which orbital is degenerate with 2p in hydrogen atom?
A. 2s
B. 3s
C. 1s
D. 3p - Q2: In multi-electron atoms, energy depends on:
A. Only n
B. Only l
C. Both n and l
D. Neither n nor l - Q3: Which has the lowest energy?
A. 3d
B. 4s
C. 4p
D. 3p
Answer Key
- Q1: A - 2s and 2p are degenerate in hydrogen.
- Q2: C - Energy depends on both n and l in multi-electron atoms.
- Q3: B - 4s has lower energy than 3d and 4p.
Memory Aids
- Energy order follows (n + l) rule.
- Degenerate orbitals have same energy in hydrogen.
- 4s fills before 3d due to lower energy.
Filling of Orbitals in Atom
Key Concepts
- Aufbau principle: Orbitals fill in order of increasing energy (1s, 2s, 2p, 3s, 3p, 4s, 3d, ...).
- Pauli exclusion principle: No two electrons have same four quantum numbers; max two electrons per orbital with opposite spins.
- Hund’s rule: Electrons fill orbitals singly first, then pair up.
Solved Examples
- Ex 1: Write the order of filling for first 10 electrons.
Answer: 1s < 2s < 2p < 3s < 3p. - Ex 2: How many electrons can occupy one orbital?
Answer: Maximum 2 with opposite spins.
Practice Set
- Q1: According to Pauli principle, maximum electrons in one orbital are:
A. 1
B. 2
C. 3
D. 4 - Q2: Hund’s rule states that:
A. Electrons pair first
B. Orbitals fill randomly
C. Orbitals fill singly before pairing
D. Electrons have same spin - Q3: Aufbau principle means:
A. Electrons fill highest energy orbitals first
B. Electrons fill orbitals in increasing energy order
C. Electrons fill orbitals randomly
D. Electrons fill orbitals based on spin
Answer Key
- Q1: B - Max 2 electrons per orbital with opposite spins.
- Q2: C - Orbitals fill singly before pairing (Hund’s rule).
- Q3: B - Orbitals fill in increasing energy order (Aufbau).
Memory Aids
- Remember: Pauli = 2 electrons max per orbital, opposite spins.
- Hund = fill singly first.
- Aufbau = fill lowest energy orbitals first.
Key Concepts
- Aufbau principle: Orbitals fill in order of increasing energy (1s, 2s, 2p, 3s, 3p, 4s, 3d, ...).
- Pauli exclusion principle: No two electrons have same four quantum numbers; max two electrons per orbital with opposite spins.
- Hund’s rule: Electrons fill orbitals singly first, then pair up.
Solved Examples
- Ex 1: Write the order of filling for first 10 electrons.
Answer: 1s < 2s < 2p < 3s < 3p. - Ex 2: How many electrons can occupy one orbital?
Answer: Maximum 2 with opposite spins.
Practice Set
- Q1: According to Pauli principle, maximum electrons in one orbital are:
A. 1
B. 2
C. 3
D. 4 - Q2: Hund’s rule states that:
A. Electrons pair first
B. Orbitals fill randomly
C. Orbitals fill singly before pairing
D. Electrons have same spin - Q3: Aufbau principle means:
A. Electrons fill highest energy orbitals first
B. Electrons fill orbitals in increasing energy order
C. Electrons fill orbitals randomly
D. Electrons fill orbitals based on spin
Answer Key
- Q1: B - Max 2 electrons per orbital with opposite spins.
- Q2: C - Orbitals fill singly before pairing (Hund’s rule).
- Q3: B - Orbitals fill in increasing energy order (Aufbau).
Memory Aids
- Remember: Pauli = 2 electrons max per orbital, opposite spins.
- Hund = fill singly first.
- Aufbau = fill lowest energy orbitals first.
Electronic Configuration of Atoms
Key Concepts
- Electronic configuration: distribution of electrons in orbitals following filling rules.
- Half-filled and fully-filled orbitals are more stable due to symmetry and exchange energy.
- Symmetry: symmetrical electron distribution increases stability.
- Exchange energy: energy released when electrons exchange positions in same subshell; max in half/full-filled subshells.
Solved Examples
- Ex 1: Why is d5 more stable than d4?
Answer: More exchange energy due to more electron exchanges. - Ex 2: What causes stability in half-filled orbitals?
Answer: Symmetry and maximum exchange energy.
Practice Set
- Q1: Which configuration is more stable?
A. d4
B. d5
C. d3
D. d2 - Q2: Exchange energy is maximum in:
A. Half-filled subshell
B. Empty subshell
C. Partially filled subshell
D. Fully filled subshell - Q3: Stability due to symmetry is because:
A. Unequal electron distribution
B. Symmetrical electron distribution
C. Random electron spins
D. No electron pairing
Answer Key
- Q1: B - d5 has maximum exchange energy and stability.
- Q2: A - Exchange energy max in half-filled subshells.
- Q3: B - Symmetry leads to greater stability.
Memory Aids
- Half-filled and full-filled orbitals = max stability.
- Exchange energy increases with electron exchanges.
- Symmetry = stability.
Key Concepts
- Electronic configuration: distribution of electrons in orbitals following filling rules.
- Half-filled and fully-filled orbitals are more stable due to symmetry and exchange energy.
- Symmetry: symmetrical electron distribution increases stability.
- Exchange energy: energy released when electrons exchange positions in same subshell; max in half/full-filled subshells.
Solved Examples
- Ex 1: Why is d5 more stable than d4?
Answer: More exchange energy due to more electron exchanges. - Ex 2: What causes stability in half-filled orbitals?
Answer: Symmetry and maximum exchange energy.
Practice Set
- Q1: Which configuration is more stable?
A. d4
B. d5
C. d3
D. d2 - Q2: Exchange energy is maximum in:
A. Half-filled subshell
B. Empty subshell
C. Partially filled subshell
D. Fully filled subshell - Q3: Stability due to symmetry is because:
A. Unequal electron distribution
B. Symmetrical electron distribution
C. Random electron spins
D. No electron pairing
Answer Key
- Q1: B - d5 has maximum exchange energy and stability.
- Q2: A - Exchange energy max in half-filled subshells.
- Q3: B - Symmetry leads to greater stability.
Memory Aids
- Half-filled and full-filled orbitals = max stability.
- Exchange energy increases with electron exchanges.
- Symmetry = stability.
NEET Chemistry — ALL CHAPTERS
1
Some Basic Concepts of Chemistry
2
Structure of Atom
3
Classification of Elements and Periodicity in Properties
4
Chemical Bonding and Molecular Structure
5
Thermodynamics
6
Equilibrium
7
Redox Reactions
8
Organic Chemistry - Some Basic Principles and Techniques
9
Hydrocarbons
10
Solutions
11
Electrochemistry
12
Chemical Kinetics
13
The d- and f- Block Elements
14
Coordination Compounds
15
Haloalkanes and Haloarenes
16
Alcohols, Phenols and Ethers
17
Aldehydes, Ketones and Carboxylic Acids
18
Amines
19
Biomolecules
20
The p-Block Elements (Group 13 and 14)
21
The p-Block Elements (Group 15 to 18)
22
Principles Related to Practical Chemistry