Power Plant Engineering
The gaseous diffusion method
Download 3.45 Mb. Pdf ko'rish
|
Power-Plant-Engineering
- Bu sahifa navigatsiya:
- 2. Thermal diffusion method.
- Fig. 10.9 3. Electromagnetic Method.
1. The gaseous diffusion method. This method is based on the principle that the diffu-
sion or penetration molecular of a gas with a given molecular weight through a porous barrier is quicker than the molecules of a heavier gas. Non-saturated uranium hexa-flouride (UF 6 ) is used for gaseous diffusion. The diffusing molecules have small difference in mass. The molecular weight of U 235 Fs = 235 + 6 × 19 = 349 and that U 238 Fs = 352. The initial mixture is fed into the gap between the porous barrier. That part of the material which passes through the barrier is enriched product, en- riched in U 235 Fs molecules and the remainder is depleted product. NUCLEAR POWER PLANT 335 2. Thermal diffusion method. In this method (Fig. 10.9) a column consisting of two concentric pipes is used. Liquid UF 6 is filled in the space between the two pipes. Temperature of one of the pipes is kept high and that of other is kept low. Due to difference in temperature the circulation of the liquid starts, the liquid rising along the hot wall and falling along the cold wall. Thermal diffusion takes place in the column. The light U 235 Fs molecules are concentrated at the hot wall and high concentration of U 236 Fs is obtained in the upper part of the column. Liquid UF 6 Enriched product Enriched product T = T 1 2 T 2 Magnetic field region Fig. 10.9 3. Electromagnetic Method. This method is based on the fact that when ions moving at equal velocities along a straight line in the same direction are passed through a magnetic field, they are acted upon by forces perpendicular to the direction of ion movement and the field. Let P = force acting on ion e = charge on ion v = velocity of ion H = magnetic field strength m = Ion mass R = radius of ion path P = euH As this force is centripetal ∴ P = 2 mv R ∴ 2 mv R = evH ∴ R = mv eH This shows that ions moving at equal velocities but different masses move along ng circumfer- ences of different radii (Fig. 10.10). Fig. 10.11 shows an electromagnetic separation unit for uranium isotopes. A gaseous uranium compound is fed into the ion source, where neutral atoms are ionised with the help of ion bombardment. The ions produced come out in the form of narrow beam after passing through a number of silos. This beam enters the acceleration chamber. These ions then enter a separation chamber where a magnetic field is applied. Due to this magnetic field the ions of different masses move along different circumference. 336 POWER PLANT ENGINEERING Ion source Accelerating electrodes H.V. Power supply Magnetic field region Collectors U 235 U 235 Filament Light molecule Heavy moelcule Download 3.45 Mb. Do'stlaringiz bilan baham: |
Ma'lumotlar bazasi mualliflik huquqi bilan himoyalangan ©fayllar.org 2024
ma'muriyatiga murojaat qiling
ma'muriyatiga murojaat qiling