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Nuclear radiations can be divided into three categories : 1. Charged particles like electr, Schemes and Mind Maps of Nuclear Physics

Nuclear radiation... A charged particle passing through neutral atoms interacts mainly by means of the Coulomb force with the electrons in the atoms. Even though in each encounter the particle loses on the average not more than a few electron Volts of kinetic energy, ionization and excitation of atoms give the greatest energy loss per unit path length of the particle. The loss of kinetic energy in a nuclear encounter would be much larger

Typology: Schemes and Mind Maps

2022/2023

Uploaded on 12/04/2023

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hiraeth-indigo ๐Ÿ‡ฎ๐Ÿ‡ถ

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Download Nuclear radiations can be divided into three categories : 1. Charged particles like electr and more Schemes and Mind Maps Nuclear Physics in PDF only on Docsity! Photoelectric Effect A gamma ray can transfer its energy to an electron originally bound in an atom because the atom can then take up some of the recoil momentum, as shown in Fig. (3.3). Conservation of momentum ๐‘ƒ๐›พ = ๐‘ƒ๐‘’ + ๐‘ƒ๐‘Ž (3.20) and Conservation of energy ๐ธ๐›พ = ๐‘‡๐‘’ +๐‘‡๐‘Ž +๐ธ๐ต (3.21) Fig. 3.3: Interaction of a gamma ray with a bound electron . can be simultaneously satisfied. In Eq. (3.21), ๐ธ๐ต is the binding energy of the electron in the atom, which is also the excitation energy of the atom after the electron has been ejected. It is not difficult to show that the recoil kinetic energy ๐‘‡๐‘Ž is of order (๐‘š0/๐‘€0) ๐‘‡๐‘’ , where ๐‘š0 ๐‘Ž๐‘›๐‘‘ ๐‘€0 are the masses of the electron and atom, respectively. Since ๐‘š0/๐‘€0 โ‰ˆ 10โˆ’4, ๐‘‡๐‘Ž can be neglected for most purposes so that ๐‘‡๐‘’ = โ„Ž๐œˆ โˆ’๐ธ๐ต (3.22) For gamma rays above about 1 2 ๐‘€๐‘’๐‘‰, photoelectrons are most probably ejected from the ๐พ ๐‘ โ„Ž๐‘’๐‘™๐‘™ of an atom because, for these electrons, the classical resonance condition is most nearly satisfied. The photoelectric effect is always accompanied by a secondary process, since the atom does not remain in its excited energy state ๐ธ๐ต. Either ๐‘ฅ โˆ’rays are emitted by the atom, or electrons are released from the outer atomic shells, which carry away the available excitation energy. These are called Auger electrons. In any dense material, the secondary radiations are absorbed in turn with a high probability. This occurs in most scintillators which are used for gamma-ray detection . Example 3.8: A 3 โˆ’ ๐‘€๐‘’๐‘‰ photon interacts by Compton scattering. (๐‘Ž) What is the energy of the photon and the electron if the scattering angle of the photon is 90ยฐ? (b) What is that energy if the angle of scattering is 180ยฐ? Solution: (๐‘Ž) ๐ธ๐›พ โ€ฒ = ๐ธ๐›พ 1+ 1โˆ’๐‘๐‘œ๐‘ ๐œƒ ๐ธ๐›พ/๐‘š๐‘2 ๐ธ๐›พ โ€ฒ = 3 1 + 1 โˆ’ 0 3/0.511 ๐ธ๐›พ โ€ฒ = 0.437 ๐‘€๐‘’๐‘‰ ๐‘‡๐‘’ = ๐ธ๐›พ โˆ’ ๐ธ๐›พ โ€ฒ ๐‘‡๐‘’ = 3 โˆ’ 0.437 = 2.563 ๐‘€๐‘’๐‘‰ (๐‘) ๐ธ๐›พ,๐‘š๐‘–๐‘› โ€ฒ = ๐ธ๐›พ 1 + 2๐ธ๐›พ/๐‘š๐‘2 = 3 1 + 2(3)/0.511 ๐ธ๐›พ,๐‘š๐‘–๐‘› โ€ฒ = 0.235 ๐‘€๐‘’๐‘‰ ๐‘‡๐‘’ = 3 โˆ’ 0.235 = 2.765 ๐‘€๐‘’๐‘‰ Example 3.9: What is the minimum energy of the ๐›พ โˆ’ray after Compton scattering if the original photon energy is 0.511, 5, 10, or 100 ๐‘€๐‘’๐‘‰? Solution: ๐ธ๐›พ,๐‘š๐‘–๐‘› โ€ฒ = ๐ธ๐›พ 1+2๐ธ๐›พ/๐‘š๐‘2 ๐‘๐‘’๐‘๐‘Ž๐‘ข๐‘ ๐‘’ ๐œƒ = 1800 for minimum energy of the ฮณ-ray after Compton scattering. The results are shown in the table below. PROBLEM 3.1 The gamma-ray photon collides with an electron at rest. It is scattered through 900, what is it frequency after collision, if itโ€™s initial frequency is (3 ร— 1019 ๐ป๐‘ง) ?
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