IPhO 2000, Теория — Задача 2. Theoretical Problem 2

XXXI International Physics Olympiad ~ Theoretical Examination — Theoretical Problem 2 (DRAFT COPY)

Условие

a) A cathode ray tube (CRT), consisting of an electron gun and a screen, is placed within a uniform constant magnetic field of magnitude B such that the magnetic field is parallel to the beam axis of the gun, as shown in figure 2.1.

Side-view schematic of a cathode ray tube: an electron gun on the left connected by a conical body to a circular screen on the right; an arrow along the axis indicates the beam direction.

The electron beam emerges from the anode of the electron gun on the axis, but with a divergence of up to 5° from the axis, as illustrated in figure 2.2. In general a diffuse spot is produced on the screen, but for certain values of the magnetic field a sharply focused spot is obtained.

Schematic showing the electron gun emitting a diverging fan of trajectories, with the extreme rays making angles of 5° above and below the central axis, converging toward a conical/screen region on the right.

By considering the motion of an electron initially moving at an angle bb (where 0≤b≤5°0 \le b \le 5°) to the axis as it leaves the electron gun, and considering the components of its motion parallel and perpendicular to the axis, derive an expression for the charge to mass ratio e/me/m for the electron in terms of the following quantities:

  • the smallest magnetic field for which a focused spot is obtained,
  • the accelerating potential difference across the electron gun VV (note that V<2V < 2 kV),
  • DD, the distance between the anode and the screen.

Write your expression in the box provided in section 2a of the answer sheet.

b) Consider another method of evaluating the charge to mass ratio of the electron. The arrangement is shown from a side view and in plan view (from above) in figure 2.3, with the direction of the magnetic field marked B. Within this uniform magnetic field B are placed two brass circular plates of radius rr which are separated by a very small distance tt. A potential difference VV is maintained between them. The plates are mutually parallel and co-axial, however their axis is perpendicular to the magnetic field. A photographic film covers the inside of the curved surface of a cylinder of radius r+sr + s, which is held co-axial with the plates. In other words, the film is at a radial distance ss from the edges of the plates. The entire arrangement is placed in vacuo. Note that tt is very much smaller than both ss and rr.

A point source of β\beta particles, which emits the β\beta particles uniformly in all directions with a range of velocities, is placed between the centres of the plates, and the same piece of film is exposed under three different conditions:

  • firstly with B=0B = 0, and V=0V = 0,
  • secondly with B=B0B = B_0, and V=V0V = V_0, and
  • thirdly with B=−B0B = -B_0, and V=−V0V = -V_0;

where V0V_0 and B0B_0 are positive constants. Please note that the upper plate is positively charged when V>0V>0 (negative when V<0V<0), and that the magnetic field is in the direction defined by figure 2.5 when B>0B>0 (in the opposite direction when B<0B<0). For this part you may assume the gap is negligibly small.

Two regions of the film are labelled A and B on figure 2.3. After exposure and development, a sketch of one of these regions is given in figure 2.4. From which region was this piece taken (on your answer sheet write A or B)? Justify your answer by showing the directions of the forces acting on the electron.

Side and plan views of the brass plates, film, field B and labelled regions A/B.
Rectangular strip of film with two curved trace lines diverging then converging between phi=0° and phi=180°, with the separation y marked at phi=90° between the two traces.

c) After exposure and development, a sketch of the film is given in figure 2.4. Measurements are made of the separation of the two outermost traces with a microscope, and this distance (yy) is also indicated for one particular angle on figure 2.4. The results are given in the table below, the angle ϕ\phi being defined in figure 2.3 as the angle between the magnetic field and a line joining the centre of the plates to the point on the film.

Angle to field /degrees ϕ\phi906050403023
Separation /mm yy17.412.79.76.43.3End of trace

Numerical values of the system parameters are given below:

B0=6.91 mTB_0 = 6.91\ \mathrm{mT}, V0=580 VV_0 = 580\ \mathrm{V}, t=0.80 mmt = 0.80\ \mathrm{mm}, s=41.0 mms = 41.0\ \mathrm{mm}

In addition, you may take the speed of light in vacuum to be 3.00×108 m s−13.00 \times 10^{8}\ \mathrm{m\,s^{-1}}, and the rest mass of the electron to be 9.11×10−31 kg9.11 \times 10^{-31}\ \mathrm{kg}.

Determine the maximum β\beta particle kinetic energy observed. Write the maximum kinetic energy as a numerical result in eV in the box on the answer sheet, section 2c.

d) Using the information given in part (c), obtain a value for the charge to rest mass ratio of the electron. This should be done by plotting an appropriate graph on the paper provided.

Indicate algebraically the quantities being plotted on the horizontal and vertical axes both on the graph itself and on the answer sheet in the boxes provided in section 2d.

Write your value for the charge to mass ratio of the electron in the box provided on the answer sheet, section 2d.

Please note that the answer you obtain may not agree with the accepted value because of a systematic error in the observations.

Решение


Оригинал в Архива: T2.pdf · официални решения: 2_sol1.jpg · допълнителни данни: 2_sol2.jpg · допълнителни данни: 2_1.png · допълнителни данни: 2_2.png · допълнителни данни: 2_3.png · допълнителни данни: T2_edited.pdf