Post on 21-Mar-2016
description
transcript
5.3.1 The Nuclear Atom
(a) describe qualitatively the alpha-particle scattering experiment and the evidence this provides for the existence, charge and small size of the nucleus (HSW)
Stow
mar
ket P
hysi
cs Alpha Particle Scattering
Stow
mar
ket P
hysi
cs Gold Foil Experiment
What were Geiger and Marsden’s results?
3. A few alpha particles were bounced back from the gold foil. 1. Most alpha particles
went straight through the gold foil, without any deflection.
2. Some alpha particles were slightly deflected by the gold foil.
Stow
mar
ket P
hysi
cs How did Rutherford interpret the results?
Rutherford had expected all the alpha radiation to pass through the gold foil. He was surprised that some alpha particles were deflected slightly or bounced back. The ‘plum pudding’ model could not explain these results, so Rutherford proposed his ‘nuclear’ model of the atom.
He suggested that an atom is mostly empty space with its positive charge and most of its mass in a tiny central nucleus.Electrons orbited this nucleus at
a distance, like planets around the Sun.
Stow
mar
ket P
hysi
cs Gold Foil Experiment
The experiment was carried out in a vacuum, so deflection of the alpha particles must have been due
to the gold foil.
How can these results be explained in terms of atoms?
Stow
mar
ket P
hysi
cs Gold Foil Experiment
Stow
mar
ket P
hysi
cs Videohttp://www.youtube.com/watch?v=u0HMYLSUzTU
(b) describe the basic atomic structure of the atom and the relative sizes of the atom and the nucleus
Stow
mar
ket P
hysi
cs Structure and size of the atomUsing Page 181 in Physics 2:
describe the basic atomic structure of the atom
and the relative sizes of the atom and the nucleus
Stow
mar
ket P
hysi
cs Structure and size of the atomAtom: protons and neutrons make up the nucleus of the atom the electrons move around the nucleus in a cloud,
some closer to and some further from the centre of the nucleus
Scale: radius of proton ~ 10-15m radius of proton ~ 10-15m radius of nucleus ~ 10-15m to 10-14m radius of atom ~ 10-10m size of molecule ~ 10-10m to 10-6m
Stow
mar
ket P
hysi
cs Structure and size of the atom… or … if the nucleus was a grape seed in the centre circle, the
electrons would be orbiting around the outside of Wembley Stadium
… or …if the nucleus was the size of a marble, the orbiting
electron would be a grain of sand 800m away… or … if the nucleus was a shopping trolley in Trafalgar
Square, the electrons would be orbiting around the M25
(c) select and use Coulomb’s law to determine the force of repulsion, and Newton’s law of gravitation to determine the force of attraction, between two protons at nuclear separations and hence the need for a short range, attractive force between nucleons (HSW)
Stow
mar
ket P
hysi
cs Forces in the nucleus
Nucleus consists of protons (+e) and neutrons Logic dictates that the +e protons should repel each
other The fact that they don’t indicates another force in the
nucleus that holds the nucleons together This force is called the strong nuclear force It only acts over small (10-14m) distances
Stow
mar
ket P
hysi
cs Forces in the nucleus
There are two other forces in the nucleus: electrostatic gravitational
The strength of each force can be calculated by: repulsive electrostatic – Coulomb’s law attractive gravitational – Newton’s laws
Stow
mar
ket P
hysi
cs Forces in the nucleus
Two protons in the nucleus of an atom are separated by 1.6 x 10-15 m.
1. Calculate the force of electrostatic repulsion between them, and the force of gravitational attraction between them.
2. Is the force of gravity enough to balance the electric repulsion tending to separate them?
3. What does this suggest to you about the forces between protons in the nucleus?
Stow
mar
ket P
hysi
cs
Newton’s law of gravitation:
where M and m = mass of each objectr = distance between each objectG = gravitational constant
Forces in the nucleus
Coulomb’s law:
where Q and q = point chargesr = distance between point charges ε0 = permittivity of free space
F = GMm r2
Stow
mar
ket P
hysi
cs Forces in the nucleus
Data:
Proton Q = 1.610-19C m = 1.6710-27kgε0 = 8.8510-12 Fm-1
G = 6.67 x 10-11 Nm2kg-2
(d) describe how the strong nuclear force between nucleons is attractive and very short-ranged
Stow
mar
ket P
hysi
cs Strong Nuclear Force
Acts over very short distances (10-14m) Attractive force Only reaches adjacent nucleons Large nucleus not held together as tightly as a small
nucleus
(e) estimate the density of nuclear matter
Stow
mar
ket P
hysi
cs Density of Nuclear Matter
Mass of proton mp = 1.67 x 10-27 kgRadius of proton r = 0.80 x 10-15 m
Volume of proton = 4 πr3
3
Density (kg m3) = mass (kg) volume (m3)
(f) define proton and nucleon number
(g) state and use the notation for the representation of nuclides
Stow
mar
ket P
hysi
cs Nucleons and electrons
Proton number:The number of protons (which is the same as number of electrons in a neutral atom).
Nucleon number:The number of protons plus the number of neutrons in a neutral atom. Element
symbol
A
X Z
(h) define and use the term isotopes
Stow
mar
ket P
hysi
cs Isotopes
All carbon atoms have the same number of protons, but not all carbon atoms are identical.
Although atoms of the same element always have the same number of protons, they can have different numbers of neutrons. Atoms that differ in this way are called isotopes.
For example, carbon exists as three different isotopes: carbon-12, carbon-13 and carbon-14:
Stow
mar
ket P
hysi
cs Isotopes
For example, carbon exists as three different isotopes: carbon-12, carbon-13 and carbon-14:
Nucleon number is different
Proton number is the same
Potassium is another element that exists as three different isotopes: potassium-39, potassium-40 and potassium-41.
Stow
mar
ket P
hysi
cs Isotopes
Isotopes are nuclei of the same element with a different number of neutrons but the same number
of protons.
Stow
mar
ket P
hysi
cs Assessment
Chapter 12 SAQ’s 1 to 11
End of Chapter 12 questions 1 - 3
Atomic Structure worksheet questions 1 – 5 and 8 – 10
(i) use nuclear decay equations to representsimple nuclear reactions
(j) state the quantities conserved in a nuclear decay.