Atoms combine to form more complex structures (compounds)
Changes to Dalton's atomic theory
1897 - Thomson discovered the electron and suggested the 'plum-pudding' model
1909 - Rutherford suggested the planetary model with a positively-chargednucleus
1913 - Bohr suggested electronsorbitthenucleus at certain distances
1932 - Chadwick discovered the neutron
1926 onwards - Schrödinger, Born and Heisenberg described electrons in terms of probability and atomic orbitals
Sub-atomic particles
Proton - Relative mass 1, Relative charge +1
Neutron - Relative mass 1, Relative charge 0
Electron - Relative mass 1/1836, Relative charge -1
Effect of electric field on sub-atomic particles
Charged particles move towards plates with opposite charge and away from plates with same charge
Electrons are deflected more than protons due to their smaller mass
Sub-atomic particles and magnetic fields
Atomic number (Z)
The number of protons in the nucleus of an atom
Mass number (A)
The number of protons plus neutrons in the nucleus of an atom
Isotopes
Atoms with the same atomic number but different mass numbers
Relative atomic mass (Ar)
The weighted average mass of naturally occurring atoms of an element on a scale where an atom of 12C has a mass of exactly 12 units
Relative isotopic mass
The mass of a particular isotope of an element on a scale where an atom of 12C has a mass of exactly 12 units
Calculating accurate relative atomic masses
1. Take into account the proportion of each isotope (relative isotopic abundance)
2. Calculate the weighted average mass
Types of radioactive emissions
Alpha (α)
Beta (β)
Gamma (γ)
Alpha (α) decay
Helium nuclei (positively charged particles) are emitted
Beta (β) decay
Electrons (produced by nuclear changes) are emitted
Gamma (γ) decay
Very high frequency electromagnetic radiation is emitted
Equations can be written for each type of radioactive decay
Uses of radioisotopes
Tracers for searching for faults and studying organs
Radiotherapy for cancer treatment
Dating objects using 14C
Smoke detectors using 241Am
Generating power using 235U
Energy quanta
The smallest fixed amount of energy required for a change
Energy levels
Certain fixed values of energy that electrons in atoms can have
The atom is most stable when the electrons are in the lowest energy levels possible (ground state)
When an electron absorbs a quantum of radiation it can move up to a higher energy level (excited state)
When an excited electron falls to a lower energy level, a quantum of radiation is given out
Relationship between energy difference and radiation frequency
ΔE = hν
Principal quantum levels/energy levels
Numbered n = 1, n = 2, n = 3, etc. going further away from the nucleus
Atomic emission spectra
Made up of separate lines
Lines converge (get closer to each other) as their frequency increases
Lyman series
Electrons fall back to the n = 1 energy level (seen in ultraviolet region)
Balmer series
Electrons fall back to the n = 2 energy level (seen in visible region)
The energy associated with each line in the emission spectrum is found using ΔE = hν
Electron
Can jump from one energy level to another by absorbing or emitting a fixed amount (quantum) of energy
Lines in the hydrogen emission spectrum get closer together
Hydrogen emission spectrum
Each line is a result of electrons moving from a higher to a lower energy level
Includes Lyman series (seen in ultraviolet region) and Balmer series (seen in visible region)
ΔE
The energy associated with each line, found using the relationship ΔE = hν
The greater the frequency (the smaller the wavelength), the more energy is released
Convergence limit
The point where the lines eventually come together, representing an electron falling from the highest possible energy level
If the electron has more energy than the convergence limit, it becomes free from the pull of the nucleus of the atom and the atom is converted to an ion
Bohr model of the hydrogen atom
The energy levels get closer together towards the outside of the atom
A quantum of energy moves the hydrogen electron in the n = 1 level (ground state) to the n = 2 level
When the electron loses energy, it will fall down to the lower energy levels, emitting radiation of characteristic frequencies
Electrons occupy specific energy levels (quantum levels) in the atom
When electrons gain specific quanta of energy they move from lower to higher energy levels. They become 'excited'
When excited, electrons lose energy, they fall back to lower energy levels emitting radiation of characteristic frequency. This is the origin of the line emission spectrum
ΔE
The energy difference between any two energy levels, given by ΔE = hν