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stars are all together. The same result is obtained from distance measurements |
by the color-brightness method. |
A study of many globular clusters gives another important bit of information. |
Tt is found that there is a high concentration oŸ such clusters in a certain part of |
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° ệ Ề k be |
c AI l sẽ. s- |
"`"... “... |
Fig. 5-6. A cluster of stars near the center of our galaxy. 'Their |
distance from the earth is 30,000 light-years, or about 3 x 1022 meters. |
the sky and that most of them are about the same distance from us. Coupling |
this Information with other evidence, we conclude that this concentration of |
clusters marks the center of our galaxy. We then know the distance to the center |
of the galaxy——about 1029 meters. |
lnowing the size of our own galaxy, we have a key to the measurement of |
stiilH larger distances—the distances to other galaxies. Eigure 5-7 is a photograph |
of a galaxy, which has much the same shape as our own. Probably it is the |
same size, too. (Other evidence supports the idea that galaxies are all about the |
same size.) IÝ it is the same size as ours, we can tell its distance. We measure |
the angle it subtends in the sky; we know its diameter, and we compute its |
distance—triangulation againl |
Photographs of exceedingly distant galaxies have recently been obtained with |
the giant Palomar telescope. One is shown in Pig. 5-8. It is now believed that |
some of these galaxies are about halfway to the limit of the universe—10”8 meters |
away——the largest distance we can contemplatel |
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`° ® * tàc . |
r 7 _< k 5 |
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T : >- £œ ° |
Fig. 5-7. A spiral galaxy like our own. Presuming that its diameter |
Is similar to that of our own galaxy, we may compute Its distance from |
its apparent size. lt is 30 million light-years (3 x 1023 meters) from the |
earth. |
5-7 Short distances |
Now lets think about smaller distances. Subdividing the meter is easy. |
'Without mụuch dificulty we can mark of one thousand equal spaces which add up |
to one meter. With somewhat more difficulty, but in a similar way (using a good |
microscope), we can mark off a thousand equal subdivisions of the millimeter |
to make a scale of microns (millionths of a meter). It ¡is dificult to continue to |
smaller scales, because we cannot “see” obJects smaller than the wavelength of |
visible light (about 5 x 10~7 meter). |
W© need not stop, however, at what we can see. With an electron microscope, |
we can continue the process by making photographs on a still smaller scale, |
say down to 10” meter (Eig. 5-9). By indirect measurements—by a kind of |
triangulation on a microscopic scale—we can continue to measure to smaller and |
smaller scales. First, from an observation oŸ the way light of short wavelength (x- |
radiation) is reflected from a pattern oŸ marks of known separation, we determine |
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k 20t § |
Ẳ° S° |
ó ° |
Fig. 5-8. The most distant object, 3C295 in BOOTES (indicated by |
the arrow), measured by the 200-inch telescope to date (1960). |
the wavelength of the light vibrations. Then, from the pattern of the scattering |
of the same light from a crystal, we can determine the relative location of the |
atoms in the crystal, obtaining results which agree with the atomic spacings aÌso |
determined by chemical means. We fñnd in this way that atoms have a diameter |
of about 10~1 meter. |
There is a large “gap” in physical sizes between the typical atomie dimension |
of about 10~10 meter and the nuclear dimensions 10~!5 meter, 10—5 times smaller. |
For nuclear sizes, a diferent way of measuring size becomes convenient. We |
measure the øpparen‡ area, ơ, called the efective cross secfion. lf we wish the |
radius, we can obtain it from ø = ør2, since nuclei are nearly spherical. |
Measurement of a nuclear cross section can be made by passing a beam of |
high-energy particles through a thin slab of material and observing the number |
of particles which do not get through. 'These high-energy particles will plow right |
through the thin cloud of electrons and will be stopped or deflected only If they |
hit the concentrated weight of a nucleus. Suppose we have a piece of material |
1 centimeter thick. There will be about 10Ẻ atomic layers. But the nuclei are |
so small that there is little chance that any nucleus will lie behind another. We |
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DISTANCES |
LIGHT-YEARS METERS |
???7?217??? |
Edge of universe |
106 To nearest neighbor galaxy |
To center of our galaxy |
To nearest star |
Radius of orbit of Pluto |
To the sun |
To the moon |
Height of a Sputnik |
Height of a TV antenna tower |
1 Height of a child |
A grain of salt |
A virus |
Radius of an atom |
10-15 Radius of a nucleus |
???7?217??? |
--- Trang 116 --- |
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