BCM.01 - ATOMS

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42 Terms

1
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Relative isotopic mass

The weighted mean mass of an atom of an isotope compared to 1/12th the mass of an atom of Carbon-12.

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Relative molecular mass

The weighted mean mass of a molecule compared to 1/12th the mass of an atom of Carbon-12

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Relative atomic mass

The weighted mean mass of an atom of an element compared to 1/12th the mass of an atom of carbon-12

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Atomic mass + unit

The mass of an isotope of an element ( Da )

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Molar mass + unit

The sum of atoms, molecules, ions or other entities in one mole of a substance in grams (gmol-1)

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Isotope

An atom of an element with the same number of protons but a different number of neutrons.

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Mole

the mass of a substance that contains 6.023 x 1023 particles of the substance.

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Dalton + value

1/12 of the rest mass of a carbon-12 atom 1.6605×10−27 kg

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Proton, Neutron and electron shorts hands

p+

n0

e-

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Specific charges on protons and neutrons

+/- 1.60 × 10-19 C

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mass of a proton

1.67 × 10-27 kg

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mass of a neutron

1.66 × 10-27 kg

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mass of an electron

1/2000

9.11 × 10-31 kg

14
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Summarise JJ Thompsons Model

If it were correct, describe the outcome of the gold foil experiment.

PLUM PUDDING MODEL

- Atoms are a ball of positive charge with tiny spheres of negative charge ( electrons ) within them, making the atom neutral.

- Alpha particles would barely be deflected due to the positive charge being diffuse and spread out over the whole volume of the atom.

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Summarise Geiger/ Mardsen/ Rutherfords model of the atom

PLANETARY MODEL

- Positive charge is concentrated at the nucleus of the atom, with electrons revolving around this nucleus in free space.

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Outline modelling subatomic interactions

- Nuclei and Alpha particle interaction can be modelled as particles. As particles have mass, momentum and velocity we can model them as small balls.

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Outline the gold foil experiment and results

H/G/R fired alpha particles at a screen of gold foil and mapped their pathways with a detector screen.

Found very few particles were significantly deflected, suggesting they were coming close to a condensed source of positive charge and were repelled ( nucleus ).

They also suggested that if the alpha particle is fired parallel to the nucleus there is a region behind the nucleus that they can never enter ( shadow ).

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Equation for density

mass/ volume

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dilution equation

C1V1=C2V2

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units of density

g.L-1

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units of molarity

mol.L-1

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1dm^3=

1L

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Usage of H,C,N,O

Basic building blocks of life

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Usage of S and P

Biochemicals - proteins and amino acids

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Alkali metals ( Na, K ) and halogens (Cl)

Electrolytes

Signalling molecules

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Transition elements ( Fe, Zn, Cu ) , Alkaline earth metals ( Ca, Mg ) and remaining non metals ( I, Se)

Trace amounts

Mg chlorophyll complex

Fe bones and blood

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Other ( B, V, Si)

B cell walls

V nitrogen fixing bacteria

( Non essential in humans )

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Why is nothing beyond Iodine used?

Elements heavier than Fe are scarce and can only be formed via supernova explosion

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Give the isotopes of Hydrogen and their percentages

H1 ( Protium ) >99%

H2 ( Deuterium - Stable )

H3 ( Tritium - Radioactive )

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Give the isotopes of Nitrogen and their percentages

N14 >99%

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Give the isotopes of Oxygen and their percentages

O16 >99%

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Give the isotopes of Carbon and their percentages

C12 99%

C13 1 % ( Used in NMR )

C14 ( Radiocarbon ) <1%

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Elements close to Fluorine are ......

Metals are .....

Electronegative

Electropositive

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Why is their more C12 in plant biomass than C13?

What can this be used for?

C12 diffuses into/ out of the stomata faster because it is lighter so is preferred. Used for finding biological origins of fossil materials.

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Unstable Isotopes ..

decay exponentially

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Equation for exponential decay

knowt flashcard image
37
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Half life, decay mode and applications of C14

5700 years

B-

Labelling

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Half life, decay mode and applications of H3

12 yrs

B-

Dating <60,000 yrs

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Half life, decay mode and applications of P32

14 days

B-

Labelling DNA/RNA

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Half life, decay mode and applications of S35

88 days

B-

Labelling proteins

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Half life, decay mode and applications K40

1.25 × 10^9 yrs

β− / e− capture + γ

Dating rocks

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Half life, decay mode and applications U235

7.04 × 10^8 yrs

α / fission

Dating rocks / power