Toner Density/Quantity Sensors Permeability sensing type TS series Type: TS-L(Double-sided substrate type) TS-A(One-sided substrate type) TS-K(One-sided substrate type) Issue date: February 2007 • All specifications are subject to change without notice. • Conformity to RoHS Directive: This means that, in conformity with EU Directive 2002/95/EC, lead, cadmium, mercury, hexavalent chromium, and specific bromine-based flame retardants, PBB and PBDE, have not been used, except for exempted applications. (1/6) Toner Density/Quantity Sensors TS-L, -A, and -K Series Conformity to RoHS Directive Plain paper copiers and laser printers require the toner (pigment powder) and carrier (magnetic powder) to be mixed in the proper proportions to create the developer. The TDK programmable toner sensor has been developed to constantly maintain the correct mix ratio between them, which is capable of keeping an optimum status by using a DC output voltage corresponding to the mix ratio. FEATURES • The TS-L, TS-A and TS-K toner sensors use a high performance ferrite core differential transformer with an adjustable control lead wires. When the DC voltage applied to the control lead wires is varied, the sensor working point also varies. Since the control lead wires (and working point) can be set to practically any desired value, it provides the following capabilities: • The sensor adjustment point can be installed at any location most convenient for operation. • Because it has such a wide control range, the working point can be reset easily after changing the developer, or whenever needed. • The microprocessor in the printer or copier can vary the control lead voltage for automatic adjustment. • In multi-color printers, it is no longer necessary to use a different constant sensor for each color. One TDK programmable toner sensor can accommodate the working point differences of each color toner with easily adjustable control voltage. • The compact size of the sensors makes them easy to install in virtually any locations. PRODUCT IDENTIFICATIONS A AND K SERIES (ONE-SIDED SUBSTRATE TYPE) ELECTRICAL CHARACTERISTICS (1) Series name (5) Sensor protrusion length(L) (2) Internal operation voltage A: 3.0mm Standard 05: 5V B: 4.5mm (3) Power supply voltage (6) Specification continuous number∗ Standard 24: 24V (7) Manufacturing internal code∗ (4) Sensor construction C: Connector type L: TH core type E: Empty sensor, etc. ∗ (6) and (7): TDK’s internal code Power supply Rated input voltage Edc(V) Power supply input current(mA) Control input Rated control input voltage Edc(V) Control input current(mA) Control input voltage range Edc(V) Control input impedance(MΩ) Analog output characteristics Output voltage B(V) Output voltage A(V) Output variable range ∆B(V) Output impedance (kΩ) Output filter time constant (s) Output ripple EP-P(mV) Temperature change(V) Digital output characteristics Digital output voltage:H (V) Digital output voltage:L(V) Digital output current:H(mA) Digital output current:L(mA) Level comparator threshold voltage (V) 24±5% 20max. 7 10max. 2 to 24 1±10% TS (1) (2) (3) (4) (5) (6) (1) Series name (2) Internal operation voltage Standard 05: 5V (3) Power supply voltage Standard 24: 24V (4) Analog output A: Analog output "Yes" N: Analog output "No" (5) Digital output D: Digital output "Yes" N: Digital output "No" (7) (8) (6) Sensor’s shape A: L type (sensing diameter: ø10mm) K: Compact type (sensing diameter: ø8mm) (7) Specification continuous number∗ (8) Manufacturing internal code∗ C: Connector type E: Empty sensor, etc. ∗ (7) and (8): TDK's internal code L SERIES (DOUBLE-SIDED SUBSTRATE TYPE) TS (1) (2) (3) (4) (5) (6) (7) 2±0.2 [at normal temperature and humidity] 3.3±0.3 [at normal temperature and humidity] 1min.[Vc:by change of 2V] 150±10% at DC 1max. 20max. ±0.5 max.[at 0 to +50°C, change from 25°C] 4.5min. 0.5max. 0.4max. 0.5max. 2.5±0.5[Analog output voltage] • The value shown above are the adjusted value of programmable toner sensors TS0524LB-X. • Conformity to RoHS Directive: This means that, in conformity with EU Directive 2002/95/EC, lead, cadmium, mercury, hexavalent chromium, and specific bromine-based flame retardants, PBB and PBDE, have not been used, except for exempted applications. • All specifications are subject to change without notice. 001-03 / 20070222 / eb372_ts.fm (2/6) SHAPES AND DIMENSIONS ONE-SIDED SUBSTRATE TYPE A SERIES DOUBLE-SIDED SUBSTRATE TYPE L SERIES 68.0±0.2 9.5±0.1 46.0±0.2 38.0±0.1 6.5±0.2 1.5 45.0±0.5 6.0±0.2 ø8.0±0.2 ø3.5±0.2 4.5±0.1 57.0±0.2 3.5 +0.1 –0 4.0±0.2 1.5±0.2 31.0±0.5 8.0±0.1 2-ø3.2×3.5 6.5±0.5 ø6.0±0.2 14.0±0.5 Label (3) 12.0±0.2 14.0±0.2 4.0±0.2 ø3.5±0.2 Label (1.5) ø10.0±0.1 Dimensions in mm ø10.0 +0 –0.1 Dimensions in mm K SERIES 63.5±0.5 55.3±0.5 Label 11.0±0.2 4.0±0.15 4.0±0.05 4.0±0.15 1.5±0.1 ø3.5±0.2 10.0±0.1 42.0±0.1 ø6.8±0.1 ø3.2±0.2 ø8 +0 –0.1 Dimensions in mm • All specifications are subject to change without notice. 001-03 / 20070222 / eb372_ts.fm (3/6) 0.01µF Control input +24V(+12V) TYPICAL CHARACTERISTICS TONER DENSITY vs. TYPICAL OUTPUT CHARACTERISTIC 5 4 Vout (V) ← Z in =1MΩ 5kΩ 50kΩ 10kΩ Power supply voltage 12V TO ADJUST WORKING POINT 3 2 Digital output 1 +24V (+12V) 0 50kΩ 0.01µF (Z out =150kΩ) 1MΩ 200kΩ TO ADJUST DIGITAL OUTPUT THRESHOLD VOLTAGE Toner density (Relative scale) CONTROL VOLTAGE VS. TYPICAL OUTPUT CHARACTERISTIC 5 4 TO INCREASE ANALOG OUTPUT FILTER TIME CONSTANT + 2 1 CNT 5V 6V 7V 8V 9V Analog output 10kΩ Analog output 3 Vout (V) (Z out =150kΩ) 2 SC 2712 (GR)etc. (H f e >200) +24V(+12V) 0 Toner density (Relative scale) TYPICAL TEMPERATURE CHARACTERISTIC TO BUFFER DIGITAL OUTPUT 5 Digital output Digital output Vout (V) 5.1kΩ 2 SC 2712 etc. 4 3 2 1 TO SWITCH WORKING POINT 0 –10 0 10 20 30 Temperatue (˚C) 40 50 60 +24V Control input TYPICAL HIGH TEMPERATURE AND HIGH HUMIDITY LOAD TEST 60˚C, 95 (%) RH Vout (V) 2.3 2.1 1.9 1.7 1.5 Initial value 72 240 Time (h) 500 1000 • All specifications are subject to change without notice. 001-03 / 20070222 / eb372_ts.fm (4/6) PRECAUTIONS Adhere to the following recommendations to ensure stable operation of the programmable toner sensor. Values shown here are guidelines for general design. Detection sensitivity of sensors is influenced by the material and shape of the developer container that the sensor will be used with, and the mechanism for carrying the developer. Refer to separate documents for special design specifications. 1. The quantity of developer (toner carrier) around the sensor face The detection sensitivity will drop when the quantity of developer around the sensor face (D in the diagram below) is low (below 5mm). Increasing the sensitivity of the sensor itself through the circuiting can compensate for this. However, as sensor sensitivity increases, environmental and temperature resistance characteristics deteriorate, causing decresed stability of operation. Design the developer container and the mechanism for carrying the developer so that there is a minimum of 6mm (D in the diagram below). Developer D Sensor face 3. Influence of conductive material near the sensor A conductive material placed near the sensor can also change its working point. If a certain distance is kept between them, normal operation can be recovered by resetting the working point. However, if the conductor is quite close to the sensor, as in the diagram below, the adjustment range for the working point may be exceeded. A D < 5mm D < 5mm A A: Conductors such as aluminum plates If the sensor is installed on a conductor such as aluminum, it may not function at all since the driving power of the sensor coil will be shorted. The custom types can be installed on conductive surfaces, but the working point adjustment will vary widely from installation to installation due to the close relationship between the mounting and the fluctuation margin of the working point. This complicates adjustment procedures. Toner sensor 2. Influence of an external magnetic field near the sensor If a DC magnetic field is applied near the sensor, the sensors working point will need to be changed correspondingly. External DC magnetic field H A A A: Conductors such as aluminum plates If the application requires installing a sensor on aluminum, working point changes can be reduced first by placing a plastic plate of at least ø30mm in diameter over the aluminum. Even with this method, some variability in working point can be expected. øD > 30mm A If the DC magnetic field strength changes depending on the individual device, the working point of the sensor will need to be reset depending on the DC magnetic field. The best environment is one where there is no DC magnetic field. However if this is unavoidable on designing, please contact us. External DC magnetic field H B B A A: Conductors such as aluminum plates B: Non-conductive material such as plastic 4. Causes of ripple of detection output Ripple in the output detection occurs when the flow rate of developer around the sensor is unstable. Depending on the size of the ripple, this can considerably lower control accuracy. For this reason it is best to locate the sensor where the flow of developer is smooth. The sensor itself contains a built-in filter for absorbing ripples, so there are generally no problems with a normal level of ripple. However if the size of the ripples exceed ordinary levels, difficulties such as those describe below may occur. If the DC magnetic field is strong, it may be necessary to use the TS-M series possessing a magnetic shield core, or the highly sensitive TS-H series with a large core for the sensor coil. As shown in the diagram above, however, the carrier that is in the developer may become trapped over the core, impairing the performance of the sensor. (The TS-L series uses a small core so this situation rarely occurs.) • All specifications are subject to change without notice. 001-03 / 20070222 / eb372_ts.fm Output (5/6) E4 P1 P2 E2 P3 E0 P6 P0 E1 E3 C2 C1 C0 P4 P5 Toner density or equivalent developer magnetic resistance C3 C4 The above illustration is a model of how unstable developer flow leads to ripple in the detection output. If there is a comparatively small fluctuation in developer flow (C0→C1→C0→C2→C0) around the working point C0, this will be reflected in an output ripple between E1 and E2. As long as the fluctuation in the output ripple remains within the developer working range, the output signal filtering is sufficient to ensure stable sensor characteristics. However, if the flow of developer fluctuates in a more unstable pattern, such as C0→C3→C0→C4→C0, the sensor saturation range may be exceeded as shown by the output ripple peaks E3 and E4. In this case sensing only takes place from P0 to P1, P2 to P3, and P5 to P6. Sensing does not take place between P1 to P2, or P4 to P5 due to saturation. Sensitivity is greatly reduced because of this. It is possible of course to reduce the ripples through filtering. However, saturation reduces the sensitivity of the sensor itself. In order to maintain the same high level of sensitivity as when there are only small ripples below saturation levels after filtering, the sensitivity needs to be increased in advance. Unfortunately, increasing the sensitivity (increasing the sensitivity to changes in the flow of developer), leads to a larger output ripple. Not only this, but as the S/N ratio does not change when sensitivity is increased, there is no increase in control accuracy, and sensor environmental characteristics are impaired as well, resulting in even more unstable sensing. What this model shows is that two sensors with the same characteristics in the working range before reaching saturation, have different outputs when there is a large ripple, causing further problems with the sensitivity of the sensors. With a large ripple, sensitivity must be adjusted individually in order to keep the output level and sensitivity of each sensor the same. This is obviously an extremely difficult task. These indicate that the problem of output ripples is not just a problem of filter characteristics, and the importance of the stable operation of each installation is emphasized. As TDK programmable toner filters are equipped with a built-in filter, any ripples that appear in sensor output are what is left after filtering. When designing the developer container it is best to temporarily remove the sensor filter so that you can view the ripples directly influenced by developer instability. 5. Relation between sensor sensitivity and sensor output voltage. TDK programmable toner sensors are set with an output center value of 2.5V for the purposes of compatibility with other applications. When the output center values of 2.5V and 5V are compared however, the 5V type has around two times the output voltage fluctuation of the 2.5V type, for the same toner density fluctuation. This shows that the 5V version has around half the sensitivity of the 2.5V version, at the same V/wt%. So the 5V type has far better environment resistance characteristics than the 2.5V type. In view of these things, the 5V type is recommended when designing a new installation. Output E2 EA EB a b C0 C1 E1(a) E1(b) Toner density or equivalent developer magnetic resistance C2 The following is another reason for avoiding large ripples. The previous diagram shows an extremely unstable case where the developer flow fluctuates between C1 and C2. In this model, two sensors, A and B are installed. Apart from having different saturation points they are identical sensors. "a" is the saturation point for sensor A, and "b" is the saturation point of sensor B. With flow fluctuating as shown (C0→C1→C0→ C2→C0), there will be two output ripples, E1(a) to E2, and E1(b) to E2. After filtering, the average output EA and EB are of course different. • All specifications are subject to change without notice. 001-03 / 20070222 / eb372_ts.fm (6/6) Phase discriminator output BASIC OPERATING PRINCIPLES (DIFFERENTIAL TRANSFORMER TYPE TONER DENSITY/QUANTITY LEVEL SENSORS) 1. OPERATING PRINCIPLE 1-2. Analog output variation by phase discriminator A toner sensor detects a toner density or residual quantity of magV2 netic developer. The developer is a magnetic material and a magnetic resistance is high if there is a small quantity of magnetic V0 (Low quantity of toner) developer and contrarily it is low if there is a large quantity of magV0 (Medium quantity of toner) netic developer. V0 (Much quantity of toner) While the toner density or quantity is obtained by detecting a magnitude of the magnetic resistance of the developer, a magnetic V3–∆V3 resistance variation is very small, thus requiring some feature V3 designed for the detection. Much quantity Low quantity V3+∆V3 1-1. Detecting principle with differential transformer type sensor L2 V2 L3 V3 V0 L1 Toner The above illustration 1-1 shows a principle diagram of a differential transformer. The differential transformer has a driving coil L1, a detecting coil L3, and a basic coil L2 in an identical core. Driving the L1 at a high frequency (500kHz) causes a differential output V0 equal to V2 minus V3 (V0 = (V2–V3)). Assuming that V30 and V20 are output voltages of the detecting and basic coils at a standard density or residual quantity and designing the transformer so that V30 equals V20, the following is obtained for a detecting coil output variation ∆V3 caused by a density/quantity variation, by which a minute variation ∆V3 is directly obtained as a differential output: V0=V20–(V30+∆V3) =–∆V3 In case of normal developer, however, ∆V3 is approx. 0.1V for a toner quantity variation of 10g around the sensor face and therefore a DC amplifier of 10 magnifications or so is required to detect it as a voltage variation, thus significantly lowering a stability of the sensor. As a means for taking an output variation without losing the stability, there is a method of discriminating a phase instead of discriminating ∆V3 as a voltage. 1-2. Differential transformer type sensor with phase discriminating method While the basic coil output V20 and the detecting coil output V30 at the standard density/quantity are set so that V30 equals V20 in order to obtain the sensor output ∆V3 in the previous section, they are set to obtain the following relation in the phase discriminating method: V20>V30 (Standard density/quantity) V20<V30+∆V3 In other words, the following relations are satisfied: V0=V20–V30>=0 (Density/low quantity or standard density /quantity) V0=V20–V30–∆V3<0 (Density/much quantity) where the phases of the differential output V0 are opposite to each other with a phase of the standard density/quantity as a boundary between them. With discriminating this phase variation using a phase discriminator, a large voltage output is obtained for a toner density/quantity variation. By slightly shifting a phase of the basic coil output voltage in advance to cause an output variation to be similar to an analog one, the output is adjusted to vary similarly to an analog output as shown in Fig. 1-2. of toner of toner 2. CIRCUIT AND OPERATION In a circuit shown in the below illustration 2-1, an EX-OR gate is used for a phase comparator, an OSC, and a wave shaping circuit: • An IC1 operates as a Colpitts OSC to drive a driving coil at approx. 500kHz. • An IC2 operates as a wave shaping inverter to shape a differential output into rectangular waves. • An IC3 operates as a phase comparator. • A C1 is a resonance capacitor, which minimize an analog output offset in case of no developer on the sensor face. • An R1 maintains an appropriate analog output sensitivity. 2-1. Circuit diagram of toner density sensor R1 Vcc 1/4 IC1 1 T 2 4 1/4 IC3 C3 R5 Analog output C4 5 3 R2 C6 R3 Digital output C2 C1 1/4 IC2 Vcc 2-2. Signal at each toner density/quantity Toner density High Middle Low 1 2 3 H 4 L Level signal • All specifications are subject to change without notice. 001-03 / 20070222 / eb372_ts.fm