First ionization energy (IE) is the energy required to remove a mole of electrons from a mole of atoms in the gaseous state to give a mole of gaseous ions, each with one positive charge
Trend in ionization energy across a period: As nuclear charge increases, electrons become harder to remove, leading to an increase in ionization energy across a period
Electrons can be thought of as a cloud of negative charge. An orbital is a way of defining the energy of an electron. Each orbital can hold two electrons of opposite spin
Protons and neutrons have approximately the same mass, so to make things easier we say they each have a mass of 1 atomic mass unit (amu). Electrons have a mass of approximately 9.11×10^-31 kg
First ionisation energy (IE) is the energy required to remove a mole of electrons from a mole of atoms in the gaseous state to give a mole positive charge
(Mass of 1st isotope × abundance 1)+ (Mass of 2nd isotope × abundance 2) + (Mass of 3rd isotope × abundance 3) ÷100
Chemical properties are determined by the number of electrons
Calculating mass of a single atom formula
Mass (g) = relativemass (g/mol) ÷ Avogadro's constant (L) which 6.022 × 10²³ mol -1
Avogadro’s constant is used to calculate how many atoms there are in one mole of any substance.
Time of Flight Mass Spectrometer stages
First the element has to be ionised this is done by two ways. One of those ways is electrospray where the sample of different elements is dissolved in a solvent. It's then pass through a fine needle with a high positive voltage. This causes an electron or more to be kicked off turning the element to an ion. The second way is electronbombardment where electrons are fired at the sample causing electrons in the sample to be knocked off and removed.
The Time of Flight Mass Spectrometer part 2
The next stage is acceleration where the now positive ions would be attracted to a negatively charged plate causing them to accelerate to it . The faster ions would be the ones with a bigger charge and a smaller mass. This is all done in an electricfield
Time of Flight mass spectrometer
The sample of ions is put into a spectrometer which is a vacuum to remove any air particles that would bump into the ions and slow then down
Time of Flight Mass Spectrometer part 3
The ions go through ion drift which is the flight path for the ions going towards the detector
Time of Flight Mass Spectrometer part 4
The ions reach the detector most at different times. The detector gives an electron or electrons to the ions this creates a current. This is proportional to their abundance of the ions
Mass number = protons + neutrons
Mass spectrometry calculations ( kinetic energy)
KE=1/2×m×v2
Where KE is kinetic energy measured in joules (J) , m is mass measured in kg and v is velocity measure in m/s