CENAC MODEL WORKING GROUP’S
REPORT
To
teach ACCELERATORS students must have acquired some previous knowledge about:
P
Magnets and charges behavior
P
Electric field
P
Forces / friction / vectors
P
Energy (equations and units)
P
Movements (velocity and acceleration)
P
Electromagnetic induction
P
Atom’s constitution
P
History of the “Search for new particles”
After the teaching, they might go thoroughly into:
Magnetic properties of
matter (atomic and nuclear magnetism) (optional)
Hall effect (measuring B
with a probe) (optional)
Superconductivity (optional)
Simple relativistic approach
(optional)
PHYSICS CONTENT |
OBJECTIVES Students must be able of… |
PROPOSED
ACTIVITIES |
The magnetic field B How does a magnetic field can
be created? Magnitude order of different B |
· Define qualitatively B · To identify and draw lines patterns of a magnetic field generated by a current · To establish the direction of a B applying Laplace law · Similarities and differences between B and E · To measure B between the poles of an electromagnet · Distinguish among different order of magnitude for physical quantities |
Simple electrical circuits to show Oersted law, relative movements of coils vs. current producing magnetic field or current Repulsion/attraction between two parallel currents Magnets attracting iron fillings / different patterns with long wire currents, solenoid, etc. Electromagnets characteristics Discharge in vaccum tubes (electron and cathode beams) deviated by a magnet To compare different magnetic field (table 1) To compare applications of different kind of accelerators (Table 2) |
The magnetic force on a moving charge Acceleration
concepts |
· Define B as a vector and a quantity ·
Units and equations of B · To establish the relationship between B and E : ; · To explain why a magnetic force on a moving charge is much more complex than an electric force on a static charge · Units of energy (joule and electron-volt) |
Mathematical approach to B and definition of the Tesla Measuring different magnetic fields in the lab, including the Earth’s using a teslameter and/or a compass
|
PHYSICS CONTENT
|
OBJECTIVES Students must be able of… |
PROPOSED
ACTIVITIES |
Accelerators concepts in particle physics research Circulating charges |
· To define/calculate Lorenz force as the resultant force dp/dt = F = Q*(E + v x B) v = E/B · To understand and apply the relationship between v, B and F · To verify that: P Trajectory curvature only due to the B field P Energy gained only due to E field · To understanding that the deflecting force has two properties that affect the trajectories of charged particles responsible for their circular motion: (1) it does not change the speed of the particles; (2) it always acts perpendicular to the velocity of the particles · To understand and use the equations.,
|
Phill
and Darren’s experiments Milikan’s experiment or Modern version of Thompson’s experiment (e/m = 2yE/B2 L2) with Helmoltz Coils CDRom by Gillies, J. and Jacobson, R. Summarized translated parts of the following lectures, with the courtesy of: - Bruning, O.- Accelerators - Schmeling, S. – HEP experiments - Rossi, L. - Superconductivity Photos from different accelerators
(Cyclotron, Synchroton), colliders, calorimeters, detectors, CERN, other
research facilities to make the transition from classroom “teaching materials”
to real life devices and events |
TABLE 1: TYPICAL
SIZES OF SOME MAGNETIC FIELDS (APPROXIMATE VALUES)
LOCATION
|
B (TESLA)
|
At
the surface of a neutron star (calculated) |
108 |
Near a superconducting magnet |
5-10 |
Near a large electromagnet |
1 |
Near
a small bar magnet |
10-2 |
At
the Earth surface |
10-4 |
In
interstellar space |
10-10 |
In
the human brain |
10-12 |
In
a magnetically shielded room |
10-14 |
In
the human heart |
10-15 |
TABLE 2 :
APPLICATIONS OF ACCELERATORS IN OUR SOCIETY
APPLICATION AREA
|
TYPE OF
ACCELERATOR
|
Magnetic field
magnitude/T
|
MEDICINE |
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INDUSTRY |
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GEOLOGY |
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RESEARCH |
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COMPARISON BETWEEN RESULTS OBTAINED WITH THE CENAC AND RESEARCH DATA….
Variable |
RESEARCH ACCELERATOR * |
CENAC MODEL (USA) |
Radius of the trajectory |
3500 m |
0,26 m |
Length of the trajectory |
27 000 m |
1,63 m |
Current ( I ) |
4 500 A |
1,5 A |
Resistance (R ) of the coil |
|
8 W |
Voltage difference |
200
kV~ |
10-12 V - |
Power (P ) dissipated |
P > 39 GW
(»
500 magnets) |
P = 18 x 4 =
72 W (4 coils) |
Friction (static)) |
Frictionless
pipes |
Fa
= 1,6 x 10 –2 N |
charge |
Charged
particles |
No charge !!! |
Particle
sources |
b-- (cathode
rays e- ) p+ (cathode tube with Hydrogen anti-matter:
pair production |
An instantaneous “push” in the “ball bearing particle” |
Mass |
Massless
/ electron and proton mass |
2,026 x 10-3
kg |
Time of one cycle |
|
2.35 s
(average) – 1,75 (min) |
Speed |
3 x 108 m/s |
0,71 m/s
(average) – 0,93 m/s (max.) |
Acceleration |
|
|
Kinetic energy |
Particle
global energy e = 0,51 MeV; p = 0,94 GeV |
|
Magnetic Field |
5 to 10 T |
2,34 – 7,87 x
10-3 T |