Light and Electromagnetic Radiation Notes
Light and Electromagnetic Radiation
Introduction
Much of our understanding of the atom's structure comes from observing how matter interacts with light.
These studies initiated quantum mechanics and aided in developing our current atom model.
Interaction of Light with Matter
When a sample absorbs visible light, the color we perceive is the sum of the remaining colors reflected or transmitted.
Opaque objects reflects light, while clear objects transmits light.
If an object absorbs all wavelengths of visible light, it appears black because no color reaches our eyes.
When sunlight (white light) passes through a prism, it separates into a spectrum of colors (ROYGBIV).
Electromagnetic Spectrum
Electromagnetic radiation involves the emission and transmission of energy through electromagnetic waves.
It encompasses radiation across a broad range of wavelengths and frequencies.
Maxwell (1873) proposed that visible light comprises electromagnetic waves.
Light, or electromagnetic radiation (same thing), is a way energy travels through space.
Concept Check:
Visible light is a type of radiation we can see, a small part of the electromagnetic spectrum.
Other types of radiation exist but are not visible to the human eye.
Electromagnetic Spectrum Ranges:
From shortest to longest wavelength:
Gamma rays (shortest)
X-rays
Ultraviolet
Visible light (400-700 nm)
Infrared
Microwaves
Radio waves (FM, Shortwave, AM) (longest)
Visible light corresponds to wavelengths between 400 and 700 nanometers (nm), covering colors from violet to red.
Visible Light Spectrum (Shortest to Longest Wavelength):
Violet: 400-420 nm (highest frequency).
Indigo: 420-440 nm.
Blue: 440-490 nm.
Green: 490-570 nm.
Yellow: 570-585 nm.
Orange: 585-620 nm.
Red: 620-780 nm (longest wavelength, lowest frequency).
All colors blend at high frequencies to produce white light.
Characteristics of Electromagnetic Radiation:
Low frequency, long wavelength, low quantum energy characterize radio waves. (violet)
High frequency, short wavelength, high quantum energy characterize gamma rays and X-rays. (red)
Wave Properties
λ (Lambda) = Wavelength: Distance between identical points on successive waves (m).
ν (Nu) = Frequency: Number of waves (cycles) per second in s^-1 or Hertz (Hz).
c = Velocity or speed of light: A constant,
approximately 3.00 × 10^8 m/s!!!
Wavelength and Frequency Relationship:
Wavelength and frequency are inversely related.
Long wavelength implies low frequency and low energy.
Model 1: Wave and Wavelength
Wavelength is the distance between two consecutive peaks or troughs of a wave.
Calculations and Conceptual Understanding:
If a wave travels at 35 cm/sec with a wavelength (λ) of 2.5 cm:
Time for one wavelength to pass point X: 2.5 cm / (35 cm/sec) ≈ 0.071 sec.
Number of wavelengths passing point X in 1 second: (35 cm/sec) / (2.5 cm) = 14λ .
If the wavelength increases, the time to travel one wavelength increases (assuming speed stays constant).
If the wavelength increases, the number of wavelengths passing a point in a given time decreases (assuming constant speed).
Frequency (ν) is the number of wavelengths passing a point per second (ν = cycles/second or Hz).
Inverse Proportionality
Wavelength and frequency are inversely proportional.
Each color of light has a characteristic wavelength and frequency.
For a wave traveling at a constant speed, frequency depends inversely on the wavelength.
Relationship between frequency, wavelength, and speed:
c = λν or λ = c/ν.
λ = nm
ν = Hertz (Hz) or s^-1
c = 3.00 × 10^8 m/s (speed of light)
True or False: For waves traveling at the same speed, longer wavelength implies greater frequency (FALSE).
Examples
Microwave ovens generate microwaves with a frequency of 2.45 × 10^9 Hz. What is the wavelength?
λ = c/ν = (3.00 × 10^8 m/s) / (2.45 × 10^9 Hz) = 0.122 m = 1.22 × 10^{-1}mWhat is the frequency of light with a wavelength of 750 nm?
λ = 750 nm = 7.5 × 10^{-7} m
ν = c/λ = (3.00 × 10^8 m/s) / (7.5 × 10^{-7} m) = 4.00 × 10^{14} Hz
Electromagnetic Radiation and Photons
Light can be considered an electromagnetic wave with a specific wavelength and frequency.
Electromagnetic waves consist of oscillating electric and magnetic fields.
The electric field oscillates in one plane (e.g., x-y plane) like a cosine wave.
The magnetic field oscillates in an orthogonal plane (e.g., x-z plane) like a cosine wave.
Einstein proposed that electromagnetic radiation could also be viewed as a stream of particles called photons.
Each photon has a particular amount of energy associated with it.
Photon Energy
E_{photon} = hν, where:
E_{photon} is the energy of a photon.
h is Planck's constant (6.63 × 10^{-34} J·s).
ν is the frequency of the radiation.
Relationship between Energy, Frequency, and Wavelength
Since ν = c/λ, the energy of a photon can also be expressed as: E_{photon} = hc/λ
Tables of Electromagnetic Radiation
Table 1: Wavelengths, Frequencies, and Energies
Wavelength (nm) | Frequency (Hz) | Energy (J) |
|---|---|---|
333.1 | 9.000 × 10^{14} | 5.963 × 10^{-19} |
499.7 | 6.000 × 10^{14} | 3.976 × 10^{-19} |
999.3 | 3.000 × 10^{14} | 1.988 × 10^{-19} |
Table 2: Regions of the Electromagnetic Spectrum
Region | Wavelength Range |
|---|---|
Radio wave | 3 km - 30 cm |
Microwave | 30 cm - 1 mm |
Infrared (IR) | 1 mm - 800 nm |
Visible (VIS) | 780 nm - 400 nm |
Ultraviolet (UV) | 400 nm - 10 nm |
X-Ray | 10 nm - 0.10 nm |
Gamma Ray | < 0.1 nm |
Units
1 nm = 10^{-9} m
1 m = 10^9 nm
The Joule (J) is a unit of energy: 1 J = 1 kg·m²/s² = 1 kPa·L = 1 N·m
Examples
A photon with a wavelength of 100 nm is classified in the ultraviolet region.
Orange light from a sodium vapor lamp has a wavelength of 589 nm. What is the energy of a single photon?
λ = 589 nm = 5.89 × 10^{-7} m
ν = c/λ = (3.00 × 10^8 m/s) / (5.89 × 10^{-7} m) = 5.09 × 10^{14} Hz
E = hν = (6.63 × 10^{-34} J·s) × (5.09 × 10^{14} Hz) = 3.38 × 10^{-19} J
Comparing the energy of red (700 nm) and blue (400 nm) photons:
Red photon:
λ = 700 nm = 7 × 10^{-7} m
ν = c/λ = (3.00 × 10^8 m/s) / (7 × 10^{-7} m) = 4.29 × 10^{14} Hz
E = hν = (6.63 × 10^{-34} J·s) × (4.29 × 10^{14} Hz) = 2.84 × 10^{-19} J
Blue photon:
λ = 400 nm = 4 × 10^{-7} m
ν = c/λ = (3.00 × 10^8 m/s) / (4 × 10^{-7} m) = 7.5 × 10^{14} Hz
E = hν = (6.63 × 10^{-34} J·s) × (7.5 × 10^{14} Hz) = 4.97 × 10^{-19} J
The blue photon is more energetic.
The Photoelectric Effect
Einstein's analysis of the photoelectric effect led him to his conclusions about light.
In the photoelectric effect, incident light ejects electrons from a material.
The photon must have sufficient energy to eject the electron.
Photoelectron spectroscopy determines the energy needed to eject electrons and provides information about the atom's structure.
The intensity of the photoelectron is a measure of the number of electrons in that energy level.
KE = hν - W, where:
KE is the kinetic energy of the ejected electron.
W is the work function, which depends on how strongly electrons are held in the metal.
Dual Nature of Light
Electromagnetic radiation exhibits both particle and wave properties.
Light travels through space as a wave and transmits energy as a particle.
De Broglie's Equation
λ = h/(mv) , where:
λ is the wavelength.
h is Planck's constant (6.63 × 10^{-34} J·s).
m is the mass of the particle.
v is the velocity of the particle.
Wavelength can be related to mass.
Combining E=mc^2 and E = hc/λ gives m = h/(λc).
For a particle not moving at the speed of light: λ = h/(mv)
Examples
An element absorbs energy at a wavelength of 150 nm, and the total energy emitted is 1.98 × 10^5 J. Calculate the number of C atoms.
Energy of a single photon: E = (6.63 × 10^{-34} J·s) × (3.00 × 10^8 m/s) / (1.50 × 10^{-7} m) = 1.33 × 10^{-18} J/photon
Number of photons: (1.98 × 10^5 J) / (1.33 × 10^{-18} J/photon) = 1.49 × 10^{23} photons
Number of C atoms: 1.49 × 10^{23} C atoms (assuming each atom emits one photon).
What is the wavelength of an electron (mass = 9.11 × 10^{-31} kg) traveling at 5.31 × 10^6 m/s?
λ = (6.63 × 10^{-34} J·s) / ((9.11 × 10^{-31} kg) × (5.31 × 10^6 m/s)) = 1.37 × 10^{-10} m = 0.137 nm
Atomic Emission Spectrum
A. Continuous Spectrum
Results when white light is passed through a prism.
Contains all wavelengths of visible light, resembling a rainbow.
Produced by sunlight or incandescent light.
A prism separates light into its constituent colors.
B. Line Spectrum
Light from a helium lamp produces discrete lines.
All elements emit light when energy is added.
Each element has a unique emission spectrum, allowing identification based on emitted colors.
Each line corresponds to a discrete wavelength.
Elements produce line spectra, not continuous spectra.
A line spectrum contains only a few lines, each corresponding to a discrete wavelength.
The type of spectrum (emission or absorption) depends on the temperature of the gas relative to the background.
C. How Elements Emit Light in the Gas State
Elements emit colors when heated or vaporized.
Electrons in atoms can only have certain allowed energies.
Heating an atom excites its electrons, causing them to jump to higher energy levels (excited state).
When electrons return to lower energy levels (ground state), they emit energy (radiation) in the form of light.
Bohr Model
Electrons in a hydrogen atom move around the nucleus in certain allowed circular orbits.
Bohr's model provided energy levels consistent with the hydrogen emission spectrum.
Ground state: The lowest possible energy state (n = 1).
Bright-line spectra confirm that only certain energies exist in the atom; the atom emits photons with definite wavelengths when the electron returns to a lower energy state.
Energy Levels
Energy levels available to the electron in an atom:
E = -2.178 × 10^{-18} J (Z^2 / n^2)
E = energy in J
Z = nuclear charge (number of protons)
n = integer related to orbital position (energy level).
Example
Calculate the energy corresponding to the n=3 electronic state in the Bohr hydrogen atom.
For hydrogen, Z = 1.
E = -2.178 × 10^{-18} J (1^2 / 3^2) = -2.42 × 10^{-19} J
Rydberg Formula
For a single electron transition in hydrogen from one energy level to another, use the Rydberg formula:
ΔE = RH (1/n{initial}^2 - 1/n_{final}^2), where:
ΔE is the energy absorbed or released.
R_H is the Rydberg constant (2.178 × 10^{-18} J).
n_{initial} is the initial energy level.
n_{final} is the final energy level.
Example
Calculate the energy change for an electron excited from n=1 to n=3 in the hydrogen atom.
ΔE = 2.178 × 10^{-18} J (1/1^2 - 1/3^2) = 1.94 × 10^{-18} J
Example
What wavelength of electromagnetic radiation is associated with this energy change?
E = hc/λ → λ = hc/E
λ = (6.63 × 10^{-34} J·s) × (3.00 × 10^8 m/s) / (1.94 × 10^{-18} J) = 1.03 × 10^{-7} m = 103 nm
Shortcomings of the Bohr Model
The model only works for hydrogen.
Electrons do not move around the nucleus in circular orbits.
Quantum Mechanical Model
We do not know the detailed pathway of an electron.
Heisenberg uncertainty principle: There is a fundamental limitation to how precisely we can know both the position and momentum of a particle at a given time.