written 5.7 years ago by |
electrostatic deflection is the method of aligning the path of charged particles by applying the electric field between the deflecting plates.
Diagram above represents the electrostatic focusing. A and B are two co-axial cylinders with potentials $V_1$ and $V_2$ such that $V_2$>$V_1$. R is the equipotential ring placed between A and B .
WORKING
(1) consider electron beam 1
It will remain normal to all equipotential surfaces and hence it is simply accelerated without any deviation of the path.
(2) consider electron beam 2
It will have following 2 effects:
(a) on the L.H.S off R
The parallel component of $F_P$ will move the electron towards right while the normal component $F_N$ will move the electron downwards by applying Fleming's left hand rule at point C.
(b) On the R.H.S off R
Fp and Fn will move the electron towards right and towards up respectively by applying Fleming's left hand rule at point D.
(3) consider electron beam 3
It's path will be as shown with same case (2)
The focal length can be changed by varying $V_1$ and $V_2$.
(4) Bethe's Law is also followed in electrostatic focusing
$v_2/v_1$ = $sin@_i/sin@_r$
(5) Electrostatic focusing is used for accelerating and focusing electron beams