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TC648 Datasheet(PDF) 12 Page - Microchip Technology |
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TC648 Datasheet(HTML) 12 Page - Microchip Technology |
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12 / 28 page ![]() TC648 DS21448C-page 12 2002 Microchip Technology Inc. Per Section 1.0, “Electrical Characteristics”, the leak- age current at the VAS pin is no more than 1 µA. It is conservative to design for a divider current, IDIV, of 100 µA. If VDD = 5.0V then… EQUATION We can further specify R1 and R2 by the condition that the divider voltage is equal to our desired VAS. This yields the following: EQUATION Solving for the relationship between R1 and R2 results in the following equation: EQUATION For this example, R1 = (2.27) R2. Substituting this rela- tionship back into the original equation yields the resistor values: R2 = 15.3 kΩ, and R1 = 34.7 kΩ In this case, the standard values of 34.8 k Ω and 15.4 k Ω are very close to the calculated values and would be more than adequate. 5.4 Output Drive Transistor Selection The TC648 is designed to drive an external transistor or MOSFET for modulating power to the fan. This is shown as Q1 in Figures 5-1, 5-6, 5-7,and 5-8. The VOUT pin has a minimum source current of 5 mA and a minimum sink current of 1 mA. Bipolar transistors or MOSFETs may be used as the power switching ele- ment, as is shown in Figure 5-6. When high current gain is needed to drive larger fans, two transistors may be used in a Darlington configuration. These circuit topologies are shown in Figure 5-6: (a) shows a single NPN transistor used as the switching element; (b) illus- trates the Darlington pair; and (c) shows an N-channel MOSFET. One major advantage of the TC648’s PWM control scheme versus linear speed control is that the power dissipation in the pass element is kept very low. Generally, low cost devices in very small packages, such as TO-92 or SOT, can be used effectively. For fans with nominal operating currents of no more than 200 mA, a single transistor usually suffices. Above 200 mA, the Darlington or MOSFET solution is recommended. For the power dissipation to be kept low, it is imperative that the pass transistor be fully sat- urated when "on". Table 5-1 gives examples of some commonly available transistors and MOSFETs. This table should be used as a guide only since there are many transistors and MOSFETs which will work just as well as those listed. The critical issues when choosing a device to use as Q1 are: (1) the breakdown voltage (V(BR)CEO or VDS (MOSFET)) must be large enough to withstand the highest voltage applied to the fan (Note: This will occur when the fan is off); (2) 5 mA of base drive current must be enough to saturate the transistor when conducting the full fan current (transistor must have sufficient gain); (3) the VOUT voltage must be high enough to suf- ficiently drive the gate of the MOSFET to minimize the RDS(on) of the device; (4) rated fan current draw must be within the transistor's/MOSFET's current handling capability; and (5) power dissipation must be kept within the limits of the chosen device. A base-current limiting resistor is required with bipolar transistors. The correct value for this resistor can be determined as follows: VOH =VBE(SAT) + VRBASE VRBASE =RBASE x IBASE IBASE =IFAN / hFE VOH is specified as 80% of VDD in Section 1.0, “Electrical Characteristics”; VBE(SAT) is given in the chosen transistor data sheet. It is now possible to solve for RBASE. EQUATION Some applications benefit from the fan being powered from a negative supply to keep motor noise out of the positive supply rails. This can be accomplished by the method shown in Figure 5-7. Zener diode D1 offsets the -12V power supply voltage, holding transistor Q1 off when VOUT is low. When VOUT is high, the voltage at the anode of D1 increases by VOH, causing Q1 to turn on. Operation is otherwise the same as in the case of fan operation from +12V. R1 + R2 IDIV = 1e –4A = , therefore 5.0V R1 + R2 = = 50,000 Ω = 50 kΩ 1e–4A 5.0V VDD x R2 R1 + R2 VAS = VDD - VAS VAS R1 = R2 x = R2 x (5 - 1.53) 1.53 VOH - VBE(SAT) RBASE = IBASE |
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