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2. Our Nearest Star |
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This is a big topic. It is split into several sections. Click on the buttons to go to the section you want. |
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The Sun
The Sun is a typical medium sized star, like thousands of millions of other stars. Light takes about 500 s to get from the Sun to us. The next star is 4.6 light years away. A light year is a unit of distance. It is the distance travelled by light, at a speed of 3 × 108 m/s, in one year.
1 light year = 3 × 108 m/s × 3600 s × 24 h × 365 dy = 1 × 1016 m (which is quite a long way)
If we went to Proxima Centauri on a fast rocket travelling at 50 000 m/s (which is motoring), it would take:
4.6 × 1016 m ÷ 50 000 m/s = 9 × 1011 s
This is about 30 000 years. We will be quite old by the time we got there.
From this you can appreciate that space is BIG.
Energy from the Sun
Like all radiations from a point source, the energy from the Sun diminishes using an inverse square law. Although the Sun is a huge object, the distances involved are so big that we can count it as a point source.
If we measure the radiation at a point r metres away from the Sun (provided we are not fried in the process), then we moved out to a point
2r metres from the Sun, we would find that the intensity would reduce to 1/4. 3r metres out, it would be 1/9 and so on. The picture shows the idea.

Here are some important terms:
Luminosity (
Energy flux (

From the definition for flux we can write:
Energy flux = total energy ÷ area
The area is the area of the sphere, so:

Luminosity varies between stars. A big star gives out more radiant energy per second than a small star. However, there is also the matter of temperature. A hotter star of the same size will give out more energy per second than a cooler star.
Black body radiation is radiant energy given off by an object. The black part is there to distinguish it from objects that have been painted. An object that is black when cold can glow red-hot or even white hot if heated enough. If we look at the radiation of a star, we see that it gives a spectrum as shown in the picture.

The colour of the 12000 K star is blue-white. There is a spread of radiation, some of which is in the visible light region. The most intense part (the peak) is in the ultra-violet region. If we look at the 6000 K star, the greatest intensity is found in the yellow region of the electromagnetic spectrum. Hence it is a yellow star (like the Sun). A yellow star still gives off UV light, so you would quickly tan if you stood by it.
You can work out the luminosity of the Sun if you equate the light of a known luminosity at a known distance. Robert Bunsen (of Bunsen burner fame) used this method.
Size and Distance
When we view an object, it subtends an angle in our eye. We call this the angular diameter. This is shown in the diagram:

From this diagram, we can see that:
d tan a = D
Therefore:
tan a = D/d
Since
D is much smaller than d, tan a (in radians) » aSo we can write:
a = D/d
It so happens that the Moon is 1/400 the diameter from the Sun and is 1/400 the distance. So the two have the same angular diameter. So in an eclipse the moon completely blacks out the disc of the Sun. When this happens, we can see that the outer atmosphere (the corona) is about twice the diameter of the Sun's disc. The Sun does not have a solid surface. Most of the radiation comes from the photosphere, the bright disc.
How old is the solar system?
Most scientists believe that the Solar System is about 4500 million years old. It is thought to have evolved from a rotating disc of gas and dust, brought together as the result of the shock wave of a supernova explosion.
Dating the solar system comes from study of the decay of radioactive isotopes.
Radiation is the process by which an unstable parent nucleus becomes more stable by decay into a daughter nucleus by emitting particles and/or energy. The basic form can be summed up as:

The decay can consist of several steps. The unstable nucleus can decay to another nucleus of a different atom by a process called transmutation. If the new nucleus is unstable it will decay again. This is known as a decay chain. There may be several steps, some of which last a very long time indeed, or can be very short. Some elements have a decay time of thousands of millions of years. In others the decay time can be microseconds.
Elements have different isotopes. An element and its isotope have:
The same
number of protons (and electrons)
Different
numbers of neutrons.
If
the isotope is unstable, it is radioactive
and is called a radioisotope.
We must be aware that radioactive decay is NOT the same as nuclear
fission.
There
are three kinds of radiation:
Alpha
– a helium nucleus
Beta – a high speed electron.
Gamma
– an electromagnetic radiation of
wavelength about 10-14 m.
These
kinds of radiation can be emitted individually or in any combination, depending
on the type of isotope that is emitting the radiation.
Often when an alpha particle is emitted the nucleus is excited
and releases the excess energy in the form of a gamma
ray or gamma photon.
When
specimens of radioactive isotopes decay they do so entirely randomly. There is no pattern whatsoever, and the rate of decay is not
affected by temperature or other physical constraints, or chemical reactions.
The
table helps us to compare the properties of radiation
|
Radiation |
Description |
Penetration |
Ionisation |
Effect of E or B field |
|
Alpha
(a) |
Helium nucleus
2p
+ 2n
Q
= + 2 e |
Few
cm air
Thin
paper |
Intense,
about 104 ion pairs per mm. |
Slight
deflection as a positive charge |
|
Beta
(b) |
High
speed electron
Q
= -1 e |
Few
mm of aluminium |
Less
intense than a, about 102 ion pairs per mm. |
Strong
deflection in opposite direction to a. |
|
Gamma
(g) |
Very
short wavelength em radiation |
Several
cm lead, couple of m of concrete |
Weak
interaction about 1 ion pair per mm. |
No
effect. |
We will look at the mechanisms of production of alpha and beta radiations:
With Alpha radiation, we generally have a big unstable nucleus. Remember that the nucleus is not a neat collection of billiard balls; it is very dynamic. Watch the animation:

You can see that the nucleus is very active. Quite by chance two neutrons and two protons are together in the same part, and are not restrained enough. The strong nuclear force is not strong enough to hold them in and they are kicked away by electromagnetic repulsion. The alpha particle is ejected from the nucleus.
Remember that the alpha is a helium nucleus, not an atom!
The nucleus is often very excited and loses the excess energy very quickly as a gamma photon.
A typical alpha decay is:

And the general equation is:

The term Q stands for energy.
Neutron
rich nuclei tend to decay by beta minus (b-) emission.
The beta particle is a high-speed electron ejected from the nucleus, NOT
the electron clouds. It is formed
by the decay of neutrons, which are slightly more energetic than a proton.
Isolated protons are stable; isolated neutrons last about 10 minutes.

The
neutron, having emitted an electron, is converted to a proton, and this results
in the proton number of the nuclide going up by 1. A new element is formed.
The reaction at the nucleon level is:

Notice
that as well as the neutron (n) and the proton (p), the beta particle is
represented as an electron (e). The
strange symbol
ne
(‘nu-bar e’) is a strange little particle called an electron antineutrino. The
general equation for
b- decay is:

A
typical decay is:

Notice
that:
The
nucleon number remains the same
The
proton number goes up by 1.
The
beta particle is created at the instant of the decay.
The
antineutrino is very highly penetrating and has a tiny mass.
It is very hard to detect.
A
precise amount of energy is released, according to the nuclide.
That
energy is shared among the nucleus, the electron and the antineutrino.
Now go on to Exponential Decay