- #1
sergiokapone
- 302
- 17
Homework Statement
The system consists of a long cylindrical anode of radius [itex]a[/itex] and a coaxial cylindrical cathode with radius [itex]b[/itex] ([itex]b <a[/itex]). On the axis of the system has a thread with a heating current [itex]I[/itex],
creates in the surrounding magnetic field.
Find the smallest potential difference between the cathode and anode, whereby thermoelectrons with zeros initial velocity will reach the anode.
Homework Equations
Equations of motion
$$\ddot{x} = \frac{e}{m}\frac{Ux}{r^2\ln{b/a}} - \frac{e}{mc}\dot{z} B_y$$
$$\ddot{y} = \frac{e}{m}\frac{Uy}{r^2\ln{b/a}} + \frac{e}{mc}\dot{z} B_x$$
$$\ddot{z} = \frac{e}{mc}(\dot{x} B_y - \dot{y} B_x)$$
and
$$\vec B = \frac{2I}{cr^2}(-y\hat e_x + x\hat e_y )$$
The Attempt at a Solution
From equation for [itex]\ddot z[/itex]I found
$$\dot z = \frac{2eI}{mc^2}\ln{\frac{r}{b}}$$
Near anode:
$$\dot z(r=a) = \frac{2eI}{mc^2}\ln{\frac{a}{b}}$$
From the Energy conservation law:
$$\frac12 m v_a^2 = eU$$
I get
$$U = \frac{2eI^2}{mc^4}\ln^2{a/b}$$
The solution in textbook is differ from above:
$$U = 2\frac{e}{m} \frac{I^2}{c^2}\ln a/b$$
Last edited: