Published:2009/7/24 5:44:00 Author:Jessie
This low-cost circuit provides line regulation (at a value set by D1) with a minimum of components. Typical values for Cin, and Co are 500μF. (View)
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Published:2009/7/24 5:43:00 Author:Jessie
This circuit provides an output (+24 V) that is double the input (+ 12 V). (View)
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Published:2009/7/24 5:42:00 Author:Jessie
This circuit provides a negative output (-5 V) with a positive input (+12 V). (View)
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Published:2009/7/24 5:41:00 Author:Jessie
The characteristics of this circuit are the same as in Fig, 4-26, except that the input can exceed 40 V, and the input/output is negative. (View)
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Published:2009/7/24 5:39:00 Author:Jessie
The characteristics of this circuit are the same as in Fig. 4-26, except that the input can exceed 40 V. (View)
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Published:2009/7/24 5:38:00 Author:Jessie
The input and output characteristics of this circuit are the same as in Fig. 4-26, except that a μA723 is used instead of an LM305. Notice that a 2N2222 is required for Q 1 . (View)
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Published:2009/7/24 5:36:00 Author:Jessie
The input and output characteristics of this circuit are the same as in Fig. 4-26, except that input and output are negative. (View)
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Published:2009/7/24 5:35:00 Author:Jessie
With the values shown, this circuit produces a±5-V output (± 1%), with a 20- to 40-V input, at currents between 2 and 10 A. mVpp (View)
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Published:2009/7/24 5:34:00 Author:Jessie
This circuit is similar to that of Figs. 4-22 and 4-24, except that there is no provision for extenal sync. The input voltage is 15 to 70 V. Typical maximum loads are 167 mA at +5V, and 33 mA at -5V. Typical minimum loads are 32 mA at + 5 V and 8 mA at -5 V. Maximum ripple is 100 mVpp. Regulation is ±5%. L1 is any 100-μH 75-mA inductor. L2 is GFS Manufacturing #85-787-4. (View)
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Published:2009/6/30 23:50:00 Author:May
The circuit provides illumination when darkness comes. By using the gain available in darlington transistors, this circuit is simplified to use just a photodarlington sensor, a darlington amplifier, and three resistors. The illumination level will be slightly lower than normal, and longer bulb life can be expected, since the D40K saturation voltage lowers the lamp operating voltage slightly. (View)
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Published:2009/7/24 9:03:00 Author:Jessie
This circuit is similar to that of Fig,4-60 In that the 2N4407 is a buffered replica of the MAX637 LX output.However,the 2N4407 has a high breakdown voltage and can be used to generate a-24-V output.The -24-V output does not appear directly on any pin of the MAX637 because it is sensed via the 1.5-MΩ external feedback resistor . (View)
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Published:2009/7/24 8:52:00 Author:Jessie
Positive-output step-up and step-down dc/dc converters have a common limitation in that neither can handle input voltages that can be both greater than (or less than) the output. For example, when convening a 12-V sealed lead-acid battery to a regulated + 12-V output, the battery voltage can vary from a high of 15 to 10 V. By using a MAX641 to drive separate P- and N-channel MOSFETs, both ends of the inductor are switched to allow noninverting buck/boost operation. A second advantage of the circuit over most boost-only designs is that the output goes to 0 V when Shutdown is activated. A drawback is that efficiency is not optimum because the two MOSFETs and diodes increase losses in the charge and discharge path of the inductor. The circuit delivers + 12 V at 100 mA with an 8-V input (70% efficiency). (View)
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Published:2009/7/24 8:50:00 Author:Jessie
By connecting a second inductor to the LX output of a MAX641 step-up dc/dc converter, the efficiency and power-handling ability can be dramatically improved. This circuit can supply 5 V at 40 mA with only 1.5-V input. With 2.4-V input, the circuit can supply 180 mA at 5 V. Notice that VOUT is not an output (in this circuit), but is the MAX641 voltage input. The pin is so labeled because VOUT is usually the output/feedback terminal of a stand-alone MAX641. (View)
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Published:2009/7/24 8:49:00 Author:Jessie
In this circuit, a +12-V input is converted to a +50 V at 50 mA by adding an IRF530 N-channel FET, which has a voltage rating of 100 V. The circuit differs from the basic MAX641 hookup in that an external resistor-divider must provide the feedback to the VFB input and that chip power comes from the + 12-V input via the VOUT pin. (View)
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Published:2009/7/24 8:47:00 Author:Jessie
The table of Fig. 4-53B lists measured efficiency of circuits using the indicated coils. In selecting coils for circuits that use external MOSFETs, it is important to calculate the peak current and to select a coil that will not saturate at that peak current. (View)
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Published:2009/7/24 8:46:00 Author:Jessie
The table of Fig. 4-52B lists the measured efficiency of circuits using the indicated coils. Efficiencies can be improved slightly by placing a Schottky diode (such as the 1N5817) in parallel with the intemal diode, from pin 4 to 5. The increase in efficiency is most noticeable for the 5-V output circuits. (View)
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Published:2009/7/24 8:44:00 Author:Jessie
This inductorless dc/dc converter generates a regulated +5 V at up to 100 mA from a single lithium cell. When powered by a DL123A (smaller than an AA cell), the circuit provides 40 mA of load current for 12 hours or more. The MAX660 in a doubler configuration steps up the battery voltage to +6 V, which is then regulated down to + 5 V by the MAX667. The surface-mount version of this circuit occupies only 1/2 square inches of PC-board space, because the circuit uses capacitors instead of inductors. The circuit capitalizes on the low dropout voltage of the MAX667 (typically less than 100 mV at 150 mA) and the 100-mA load capability and 95% efficiency of the MAX660. (View)
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Published:2009/7/24 8:43:00 Author:Jessie
In this circuit, a MAX660 charge pump is used as a voltage inverter, creating a negative voltage of approximately equal magnitude to the input voltage. Although the MAX660 has no feedback mechanism, and so is unregulated, the output is a stiff, accurate supply when operated from a regulated input. An output current of 100 mA results in a typical voltage loss of 0.65 V (the drop at 10 mA is less than 100 mV). The FC input selects a 10- or 45-kHz oscillator frequency. Notice that this circuit provides an optional shutdown that disables the internal oscillator, and reduces the supply current to less than 1μA. (View)
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Published:2009/7/24 8:41:00 Author:Jessie
This circuit controls four loads via low on-resistance N-channel MOSFETs. If all four switches are programmed off, the power supply input to the MAX620 is disconnected, and the standby supply drain is reduced to 2μA. (View)
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Published:2009/6/30 23:39:00 Author:May
The circuit uses a free-running push-pull dc to dc high voltage converter to get the necessary voltage for the laser plasma tube supply. The supply voltage VC of this converter, is adjusted by a switch-mode power supply in order to keep the load current constant, at set value. The linear opto-electronic isolator U2, connected in series with the laser plasma tube, gives a voltage VF proportional to the discharge current ID across R18, having the correct polarity to drive directly the inverting input of U1, D7, R15 protects the optoisolator diode against damage produced by the high voltage ignition pulse.Due to the high operating frequency of the high voltage converter (25 kHz) the ripple of the laser output power is less than 2.10-4. The stability of ID is better than 10-2, for variations of supply voltage VS is the range of ±10%, and depends on the optoisolator sensitivity. (View)
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