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of frequency Acs/cooof the photon at a very great distance from the star. 5.270. A voltage applied to an X-ray tube being increased ri = = 1.5 times, the short-wave limit of an X-ray continuous spectrum shifts by Ak = 26 pm. Find the initial voltage applied to the tube. 5.271. A narrow X-ray beam falls on a NaC1 single crystal. The least angle of incidence at which the mirror reflection from the system of crystallographic planes is still observed is equal to a = = 4.1°. The interplanar distance is d = 0.28 nm. How high is the voltage applied to the X-ray tube? 5.272. Find the wavelength of the short-wave limit of an X-ray continuous spectrum if electrons approach the anticathode of the tube with velocity v = 0.85 c, where c is the velocity of light. 5.273. Find the photoelectric threshold for zinc and the maximum velocity of photoelectrons liberated from its surface by electromag- netic radiation with wavelength 250 nm. 5.274. Illuminating the surface of a certain metal alternately with light of wavelengths X1 = 0.35 tim and XI= 0.54 lam, it was found that the corresponding maximum velocities of photoelectrons differ by a factor 2.0. Find the work function of that metal. 5.275. Up to what maximum potential will a copper ball, remote from all other bodies, be charged when irradiated by electromagnetic radiation of wavelength k = 140 nm? 5.276. Find the maximum kinetic energy of photoelectrons liberat- ed from the surface of lithium by electromagnetic radiation whose electric component varies with time as E = a (1 + cos cot) cos coot, where a is a constant, co = 6.0.1014 s-1and coo= 3.60.1015 s-. 5.277. Electromagnetic radiation of wavelength? = 0.30 Rm falls on a photocell operating in the saturation mode. The correspond- ing spectral sensitivity of the photocell is J = 4.8 mA/W. Find the yield of photoelectrons, i.e. the number of photoelectrons produced by each incident photon. 5.278. There is a vacuum photocell whose one electrode is made of cesium and the other of copper. Find the maximum velocity of photoelectrons approaching the copper electrode when the cesium electrode is subjected to electromagnetic radiation of wavelength 0.22 p.m and the electrodes are shorted outside the cell. 5.279. A photoelectric current emerging in the circuit of a va- cuum photocell when its zinc electrode is subjected to electromagnetic radiation of wavelength 262 nm is cancelled if an external decelerat- ing voltage 1.5 V is applied. Find the magnitude and polarity of the outer contact potential difference of the given photocell. 5.280. Compose the expression for a quantity whose dimension is length, using velocity of light c, mass of a particle m, and Planck's constant /1. What is that quantity? 5.281. Using the conservation laws, demonstrate that a free electron cannot absorb a photon completely.
5.282. Explain the following features of Compton scattering of light by matter: (a) the increase in wavelength AA, is independent of the nature of the scattering substance; (b) the intensity of the displaced component of scattered light grows with the increasing angle of scattering and with the diminish- ing atomic number of the substance; (c) the presence of a non-displaced component in the scattered radiation. 5.283. A narrow monochromatic X-ray beam falls on a scattering substance. The wavelengths of radiation scattered at angles 01= 60° and 02= 120° differ by a factor ri = 2.0. Assuming the free electrons to be responsible for the scattering, find the incident radiation wave- length. 5.284. A photon with energy ho) = 1.00 MeV is scattered by a stationary free electron. Find the kinetic energy of a Compton electron if the photon's wavelength changed by 11 = 25% due to scattering. 5.285. A photon of wavelength X = 6.0 pm is scattered at right angles by a stationary free electron. Find: (a) the frequency of the scattered photon; (b) the kinetic energy of the Compton electron. 5.286. A photon with energy how = 250 keV is scattered at an angle 0 = 120° by a stationary free electron. Find the energy of the scattered photon. 5.287. A photon with momentum p = 1.02 MeV/c, where c is the velocity of light, is scattered by a stationary free electron, changing in the process its momentum to the value p' = 0.255 MeV/c. At what angle is the photon scattered? 5.288. A photon is scattered at an angle 0 = 120° by a stationary free electron. As a result, the electron acquires a kinetic energy T = (^) 0.45 MeV. Find the energy that the photon had prior to scat- tering. 5.289. Find the wavelength of X-ray radiation if the maximum kinetic energy of Compton electrons is T,,,„„ = 0.19 MeV. 5.290. A photon with energy hco = 0.15 MeV is scattered by a stationary free electron changing its wavelength by AX = 3.0 pm. Find the angle at which the Compton electron moves. 5.291. A photon with energy exceeding ri = 2.0 times the rest energy of an electron experienced a head-on collision with a sta- tionary free electron. Find the curvature radius of the trajectory of the Compton electron in a magnetic field B = 0.12 T. The Compton electron is assumed to move at right angles to the direction of the field. 5.292. Having collided with a relativistic electron, a photon is deflected through an angle 0 = 60° while the electron stops. Find the Compton displacement of the wavelength of the scattered photon.
(a) the least curvature radius of its trajectory; (b) the minimum approach distance between the particle and the nucleus.
deflected by the Coulomb field of a stationary Au nucleus. Find the momentum imparted to the given nucleus as a result of scattering.
acquired by the electron, assuming the proton's trajectory to be rectilinear and the electron to be practically motionless as the proton flies by.
the potential energy of the particle takes the form
where r is the distance from the centre of the well. Find the relation-
through which it deflects from the initial motion direction.
a particle and the ball to be elastic, find: (a) the deflection angle 0 of a particle as a function of its aiming
(b) the fraction of particles which after a collision with the ball are scattered into the angular interval between 0 and 0 + d0; (c) the probability of a particle to be deflected, after a collision with the ball, into the front hemisphere (0 <
6.9. A narrow beam of alpha particles with kinetic energy 1.0 MeV falls normally on a platinum foil 1.0 μm thick. The scattered par- ticles are observed at an angle of 60° to the incident beam direction by means of a counter with a circular inlet area 1.0 cm2located at the distance 10 cm from the scattering section of the foil. What fraction of scattered alpha particles reaches the counter inlet?
normally on a golden foil. Find the thickness of the foil if at a distance r = 15 cm from a scattering section of that foil the flux density of scattered particles at the angle 0 = 60° to the incident beam is
6.11. A narrow beam of alpha particles falls normally on a silver foil behind which a counter is set to register the scattered particles. On substitution of platinum foil of the same mass thickness for the silver foil, the number of alpha particles registered per unit time increased = 1.52 times. Find the atomic number of platinum,
assuming the atomic number of silver and the atomic masses of both platinum and silver to be known. 6.12. A narrow beam of alpha particles with kinetic energy (^) T = = 0.50 MeV falls normally on a golden foil whose mass thickness is pd = (^) 1.5 mg/cm2. The beam intensity is / 0= 5.0.105particles per second. Find the number of alpha particles scattered by the foil during a time interval -r = 30 min into the angular interval: (a) 59-61°; (b) over 00= 60°. 6.13. A narrow beam of protons with velocity v = 6.106 m/s falls normally on a silver foil of thickness d = 1.0 p,m. Find the probability of the protons to be scattered into the rear hemisphere (0 > 90°). 6.14. A narrow beam of alpha particles with kinetic energy T = = 600 keV falls normally on a golden foil incorporating n = 1.1.1019nuclei/cm2. Find the fraction of alpha particles scattered through the angles 0 < 00= 20°. 6.15. A narrow beam of protons with kinetic energy (^) T = 1.4 MeV falls normally on a brass foil whose mass thickness pd = 1.5 mg/cm2. The weight ratio of copper and zinc in the foil is equal to 7 : 3 re- spectively. Find the fraction of the protons scattered through the angles exceeding 00= 30°. 6.16. Find the effective cross section of a uranium nucleus cor- responding to the scattering of alpha particles with kinetic energy T = 1.5 MeV through the angles exceeding 00= 60°. 6.17. The effective cross section of a gold nucleus corresponding to the scattering of monoenergetic alpha particles within the angular interval from 90° to 180° is equal to Au = 0.50 kb. Find: (a) the energy of alpha particles; (b) the differential cross section of scattering doldS2 (kb/sr) cor- responding to the angle 0 = 60°. 6.18. In accordance with classical electrodynamics an electron moving with acceleration w loses its energy due to radiation as
dE 2e 2 2 dt - 3c3 W '
where e is the electron charge, c^ is the velocity of light. Estimate the time during which the energy of an electron performing almost harmonic oscillations with frequency co = 5.1015 s-1will decrease = 10 times. 6.19. Making use of the formula of the foregoing problem, estimate the time during which an electron moving in a hydrogen atom along a circular orbit of radius r = 50 pm would have fallen onto the nucleus. For the sake of simplicity assume the vector w to be perma- nently directed toward the centre of the atom. 6.20. Demonstrate that the frequency co of a photon emerging when an electron jumps between neighbouring circular orbits of a hydrogen-like ion satisfies the inequality con> co > con +1, where conand con +1are the frequencies of revolution of that electron around