108D12GY119 — Single-Beam Oscilloscope Tube
The 108D12GY119 is a single-beam, single-acceleration electrostatic cathode-ray tube designed for use in oscilloscopes with bandwidths up to 25 MHz, such as portable service oscilloscopes and display units. It features a rectangular flat screen with a 12 cm diagonal, an integrated low-power heater cathode, and a permanently mounted correction coil for image rotation.
Mechanical Design and Screen Characteristics
The tube is constructed with a rectangular, planoparallel front plate. The screen utilizes a GY-type green phosphor with medium persistence. An internal, illuminable red graticule is integrated directly onto the screen, featuring a 10 x 8 division layout based on an 8 mm grid. The graticule lines have a width of 0.2 mm, and the intersection points have a diameter of 0.4 mm. The planoparallel front plate features a ground edge designed for the lateral coupling of floodlight illumination to light the internal graticule.
To facilitate precise alignment of the internal graticule when mounting the tube into an oscilloscope front mask, three physical stop points (designated A, B, and C) are located on the edges of the close-tolerance front plate. The position of the internal graticule is directly referenced to these points. Because the glass seal seam is visible through the front plate and is not necessarily aligned with the internal graticule, the use of a front mask with an opening of 82 mm x 66 mm is recommended. The front plate, cone, and seal seam are designed to fit through a chassis opening of 101 mm x 85 mm.
Physical Dimensions and Mounting
During installation, the tube must be mounted in a manner that prevents any mechanical stress on the glass bulb or the socket. The socket must never be used as a structural support to hold the weight of the tube.
Electron Gun and Deflection System
The 108D12GY119 utilizes an indirectly heated, low-power cathode (Sparheizkatode) designed for parallel supply using either alternating or direct current.
Heater Characteristics
The tube features electrostatic focusing and double-electrostatic, symmetrical deflection. A built-in permanent-magnetic electron-optical lens system is integrated to correct angular deviations between the horizontal and vertical deflection axes (orthogonality), vertical deviation (eccentricity), and astigmatism of the electron spot.
The nominal angle between the horizontal and vertical deflection directions is 90°. The angle between the horizontal deflection direction and the horizontal centerline of the internal graticule is a maximum of 5° (which can be corrected via the integrated coil). The undeflected spot may deviate from the physical center of the internal graticule by a maximum of 4 mm horizontally and 2 mm vertically. Deflection non-linearity is limited to a maximum of 2%, measured at 25% and up to 75% of the usable deflection area.
Interelectrode Capacitances
Electrical Ratings and Operating Conditions
The operating and maximum ratings of the 108D12GY119 are specified relative to the cathode unless otherwise noted.
Absolute Maximum Ratings (Grenzdaten)
Typical Operating Data (Betriebsdaten)
At typical operating points, the voltages are set as follows for optimal geometry:
The usable screen area is at least 82 mm x 66 mm, while the usable deflection area is at least 80 mm x 64 mm.
Integrated Correction Coil
The tube features a factory-installed correction coil secured to the neck using synthetic resin adhesive and adhesive tape. This coil is designed to correct rotational alignment errors of the displayed image.
Correction Coil Parameters
The maximum correction voltage of approximately 11 V is sufficient to compensate for a tube alignment tolerance of up to ±5∘ combined with a geomagnetic residual field of up to ±2∘ (assuming reasonable external shielding is used).
Circuit Integration and Optimization
To maintain proper raster geometry and prevent distortion, the horizontal and vertical deflection plates must be driven with symmetrical deflection voltages. Unsymmetrical operation will degrade the raster geometry.
Deflection Plate Potential Alignment
For minimal adjustment effort during oscilloscope calibration, the mean potential of the horizontal deflection plates should equal the mean potential of the vertical deflection plates. Under this condition, the screen electrode G5 can be connected directly to the accelerator electrodes G2 and G4, and biased to the mean potential of the vertical deflection plates to achieve optimal spot shape.
A potential difference of less than 75 V between the mean potentials of the horizontal and vertical deflection plates is permissible. However, such a difference can alter the deflection coefficients and may require a separate, dedicated voltage supply for the screen electrode G5 (set equal to the mean potential of the horizontal deflection plates) to correct the raster geometry.
If the screen electrode voltage UG5 is kept equal to the mean potential of the horizontal deflection plates, the raster geometry deviations will remain within specified tolerances. Providing an adjustment range of ±50 V relative to the mean potential of the horizontal deflection plates allows for fine-tuning of the raster geometry.
Spot Shape and Focus Optimization
An optimal spot shape is achieved when the acceleration voltage U[G2](/tubes/G2),G4 is equal to the mean potential of the vertical deflection plates. Small deviations of up to ±4 V generally do not cause any visible degradation of the spot shape. As the screen electrode voltage UG5 is increased, the required acceleration voltage U[G2](/tubes/G2),G4 shifts toward lower values. The acceleration voltage U[G2](/tubes/G2),G4 must be supplied from a low-impedance source with an internal resistance of less than 10 kΩ.
To simplify the adjustment of the spot shape, the voltage swing of the focus control on the oscilloscope front panel should be limited to 30 V. The required focusing voltage UG3 decreases as the grid drive voltage U1 increases.
Intensity Control and Beam Loading
The voltage swing of the intensity control on the front panel should be limited to prevent the screen current IL from exceeding its maximum useful value of approximately 50 μA. This limit is typically reached at a grid drive voltage of up to 22 V, or when the maximum acceptable line width is reached.
The cathode current IK or the accelerator electrode current I[G2](/tubes/G2),G4 (which can reach up to 500 μA) cannot be used directly to set or calibrate the intensity. These currents are highly dependent on the specific control grid voltage −UG1 required for visual spot extinction.
Furthermore, because the electron beam can graze the deflection plates at full deflection, the deflection amplifiers driving the plates must feature a low output impedance.
Technical Summary
The 108D12GY119 is a specialized, single-beam, electrostatic-deflection oscilloscope tube featuring a 12 cm rectangular flat screen with a green, medium-persistence GY phosphor. Operating with a nominal screen and acceleration potential of 2000 V, it provides a highly legible display with an integrated red graticule. The tube incorporates a low-power 6.3 V, 100 mA heater, electrostatic focusing, and an integrated 1000-turn correction coil to compensate for up to ±5∘ of rotational misalignment. With horizontal and vertical deflection coefficients of 19 V/div and 11 V/div respectively, and a design optimized for symmetrical drive, it is well-suited for high-precision portable service oscilloscopes and display systems operating at bandwidths up to 25 MHz.