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TELTRON TUBES (Original style tubes still available. Call for prices.) INTRODUCTION | FINE BEAM TUBE | LARGE DIAMETER FINE BEAM e/m TUBE | PLANAR DIODE | PLANAR TRIODE | GAS-FILLED (HE or NE) PLANAR TRIODE | LARGE DIAMETER FINE BEAM e/m TUBE | MALTESE CROSS | LUMINESCENT TUBE | PERRIN TUBE |
Knowledge of the electron is fundamental to understanding atomic structure. Part of this knowledge is knowing the electron's constants. J. J. Thomson, nearly a century ago, successfully measured the charge-to-mass ratio of an electron. Within 20 years Millikan carefully determined the charge of the electron thus enabling its mass to be calculated. With the Thomson e/m Tube you can perform this important classical experiment to determine the charge-to-mass ratio of the electron. The Thomson e/m Tube is an evacuated tube in which a scale is printed on one side of a semitransparent square mica card. This card is held in place by two metal plates which can provide an Electric Field, E. Helmholtz Coils held in place by the Universal Stand can then provide a Magnetic Field, B at right angles to the Electric Field. A phosphor on the opposite side of the mica card will show the parabolic path of the electron beam in an Electric Field and the circular path of the beam in a Magnetic Field (see figure 2). A beam of electrons is generated from a hot filament. This beam is accelerated through the Magnetic and Electric Fields which are at right angles to each other and in a path that is perpendicular to the Electric Field. Using the kinetic energy formula 1/2mv2 and the Lorentz equation F=eE+evXB, (which describes the force on a charged particle in a Magnetic and Electric Field), permits one to calculate e/m. You can determine e/m using Thomson's method. You can also calculate e/m by using just the Magnetic Field.
THE COMPLETE E/M SYSTEM includes: TEL 2014 Power Plug TEL 2501 Universal Stand TEL 2502 Helmholtz Coils TEL 2525 Thomson e/m Tube TEL GP4303D Power Unit TEL EV14 Power Unit TEL 2811 HiVoltage Bias
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Fig.1 TEL 2525 THOMSON e/m TUBE WITH TEL 2501 UNIVERSAL STAND
AND TEL 2502 HELMHOLTZ COILS AND THE TEL 2811
HIVOLTAGE BIAS
FIG. 2: TEL 2525 SHOWING AN ELECTRON IN A MAGNETIC FIELD
FIG. 3: PATH OF AN ELECTRON IN BALANCED PERPENDICULAR
MAGNETIC & ELECTRIC FIELDS
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