Presentation on theme: "Applications of the Motion of Charged Particles in a Magnetic Field AP Physics C Montwood High School R. Casao."— Presentation transcript:
Applications of the Motion of Charged Particles in a Magnetic Field AP Physics C Montwood High School R. Casao
Lorentz Force In many devices that involve the motion of charged particles in uniform magnetic fields, the charge under consideration will be moving with velocity v in the presence of both an electric field E and a magnetic field B. The charge will experience both an electric force q·E and a magnetic force q·(v × B). The total force, called the Lorentz force, on the charge is:
Velocity Selector Experiments involving the motion of charged particles often require particles that move in a straight line with the same velocity. A combination of an electric field and a magnetic field can produce this stream of particles. A uniform electric field E is provided by a pair of charged parallel plates. A uniform magnetic field B is applied perpendicular to E such that F mag is equal to and opposite to F electric.
The two fields, called crossed fields can be manipulated to produce velocities in other directions.
Mass Spectrometer Separates atomic and molecular ions based on their mass-to-charge ratio. A beam of ions first passes through a velocity selector and then enters a uniform magnetic field B o, where the ions move in a semicircle of radius r before striking a photographic plate at P. Mass-to-charge ratio:
If the magnetic field in the velocity selector is B, then: Charge-to-mass ratio for electrons: –Electrons are accelerated from the cathode to the anode, passing through slits in the anodes, and allowed to drift into a region of perpendicular electric and magnetic fields. –The crossed fields are first adjusted to produce an undeflected beam.
The magnetic field B is turned off and the electric field E produces a measureable beam deflection on the screen. From the size of the deflection and the values for E and B, the charge-to-mass ratio can be determined.
Cyclotron Cyclotron accelerates charged particles to very high velocities using both electric and magnetic fields. The high energy particles that emerge from the cyclotron are used to bombard other nuclei to produce nuclear reactions for researchers to study. Hospitals use cyclotrons to produce radioactive substances used in diagnosis and treatment.
Motion of the charges occurs in two semicircular containers D 1 and D 2 (called dees).
The dees are evacuated to prevent energy losses in collisions with the ions and air molecules. A high frequency alternating voltage is applied to the dees and an electromagnet provides a uniform magnetic field directed perpendicular to the dees. Positive ions released at P near the center of the electromagnet move in a semicircle and arrive back at the gap in a time T/2. The frequency of the applied voltage is adjusted so that the polarity of the dees is reversed in the same time it takes for the ions to complete one half of a revolution.
If the phase of the applied voltage is adjusted so that D 2 is a a lower potential than D 1 by an amount V, the ion will accelerate across the gap to D 2 and its kinetic energy will increase by an amount q·V. Ion continues to move in D 2 in a semicircular path of larger radius due to the velocity increase. After a time T/2 it arrives at the gap.
The voltage across the gap is reversed so that D 1 is now negative and the ion is again accelerated across the gap. The ion is accelerated at each half revolution, gaining a kinetic energy equal to q·V each time. When the radius of the orbit is nearly that of the dees, the ion leave the system through an exit slit. The maximum kinetic energy of the ion can be obtained upon the exit of the ion from the cyclotron: Frequncy of oscillation of the cyclotron:
Period: Angular frequency (rad/s): Cyclotron frequency (Hz):
When the cyclotron principle is used to accelerated electrons, it has been historically called a betatron. The cyclotron principle as applied to electrons is illustrated below.
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