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Structure of the Atom Reading
Structure of the Atom Reading

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InorgCh2.1

Name Period Nuclear Study Packet Set 1 1. What subatomic
Name Period Nuclear Study Packet Set 1 1. What subatomic

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... electron's momentum is ∆pelectron and certainly it is proportional to pphoton. Let us assume the constant of proportionality to be 1 in the present context. Thus, ∆pelectron = h/λ. Now the precision with which we can determine a distance is limited by the size of the wavelength λ of the light which ...
CHAPTER 4: Structure of the Atom
CHAPTER 4: Structure of the Atom

The stability of an atom depends on the ratio and number of protons
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... chemical properties; as is apparent among other series in that of Li, Be, B, C, N, O, and F. 4. The magnitude of the atomic weight determines the character of the element, just as the magnitude of the molecule determines the character of a compound body. 5. We must expect the discovery of many yet u ...
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... through a magnetic field. Some of the radioactivity was deflected to the positive plate; some of it was deflected to the negative plate; and the rest went through the magnetic field without deflection. Thus, there were three types of radioactivity: alpha particles (+), beta particles (-) and gamma r ...
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Chapter 30: The Nature of the Atom Very schematic picture of an atom
Chapter 30: The Nature of the Atom Very schematic picture of an atom

... • Electrons orbit a positively-charged nucleus. • The electrons suffer centripetal acceleration in their orbits. • Any accelerated charge should radiate electromagnetic energy. " The electrons should lose energy and spiral into the nucleus in very ...
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Geiger–Marsden experiment



The Geiger–Marsden experiment(s) (also called the Rutherford gold foil experiment) were a landmark series of experiments by which scientists discovered that every atom contains a nucleus where its positive charge and most of its mass are concentrated. They deduced this by measuring how an alpha particle beam is scattered when it strikes a thin metal foil. The experiments were performed between 1908 and 1913 by Hans Geiger and Ernest Marsden under the direction of Ernest Rutherford at the Physical Laboratories of the University of Manchester.
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