Given: "U=100 V" ; "d=5mm=5.0\\cdot 10^{-3}V"; "B=0.01T=10^{-2}T"
Solution: In the problem, the motion of electrons occurs in electric and magnetic fields. In this case, two forces exert on a charged particle, these are Coulomb "\\vec F_c=e\\cdot \\vec E" and Lorentz "\\vec F_l=e\\cdot[\\vec v\u0445\\vec B]" forces. Since an electron beam passes un deflected with uniform velocity "\\vec v" these two forces compensate each other. We may choose a coordinate system so that the electric field is directed perpendicular to plates along "\\hat k" ("\\vec E=E\\cdot \\hat k" ), the magnetic field is directed along "\\hat j" ("\\vec B=B\\cdot \\hat j" ) parallel plates and the velocity of electrons is directed along parallel plates too, say "\\vec v=v_x\\hat i+v_y\\hat j" . If we calculate the Lorentz force,
(1) "\\vec F_l=e\\cdot \\begin{pmatrix} \\hat i & \\hat j & \\hat k\\\\ v_x & v_y &0\\\\0& B &0 \\end{pmatrix}=e\\cdot(v_x B\\cdot \\hat k)" we will see that the Lorentz force disappears for movement along the magnetic field. Therefore, if the electrons had a velocity component "v_y\\not =0" they would move in the Y direction without Lorentz force, and a Lorentz force could not compensate the electric force. Therefore, we must put "v_y=0" and the movement of electrons occurs only along X direction. Subject to compensation of forces we have
"\\vec F_c=\\vec F_l" The charge of partical is reduced, the directions of forces are coincide and we get
(2) "E=v_xB" or "v_x=\\frac{E}{B}"
The field "E" of parallel plates condenser can be calculated by the formula
(3)"E=\\frac {U}{d}=\\frac{100V}{5\\cdot 10^{-3}m}=2\\cdot10^4 V\/m"
Substituting (3) into (2) we get finally
"v_x=\\frac{2\\cdot 10^4V\/m}{10^{-2}T}=2\\cdot 10^6 m\/s"
Answer: the velocity of beam is "2\\cdot 10^6 m\/s"
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