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LT1010CDD датащи(PDF) 7 Page - Linear Technology |
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LT1010CDD датащи(HTML) 7 Page - Linear Technology |
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7 / 20 page ![]() 7 LT1010 1010fc APPLICATIO S I FOR ATIO General These notes briefly describe the LT1010 and how it is used; a detailed explanation is given elsewhere1. Empha- sis here will be on practical suggestions that have resulted from working extensively with the part over a wide range of conditions. A number of applications are also outlined that demonstrate the usefulness of the buffer beyond that of driving a heavy load. Design Concept The schematic below describes the basic elements of the buffer design. The op amp drives the output sink transis- tor, Q3, such that the collector current of the output follower, Q2, never drops below the quiescent value (de- termined by I1 and the area ratio of D1 and D2). As a result, the high frequency response is essentially that of a simple follower even when Q3 is supplying the load current. The internal feedback loop is isolated from the effects of capacitive loading by a small resistor in the output lead. R1 D2 I2 D1 A1 Q3 INPUT OUTPUT V+ V– 1010 AI01 BIAS I1 Q1 Q2 idealized buffer with the unloaded gain specified for the LT1010. Otherwise, it has zero offset voltage, bias current and output resistance. Its output also saturates to the internal supply terminals2. 1R. J. Widlar, “Unique IC Buffer Enhances Op Amp Designs; Tames Fast Amplifiers,” Linear Technology Corp. TP-1, April, 1984. 2See electrical characteristics section for guaranteed limits. The scheme is not perfect in that the rate of rise of sink current is noticeably less than for source current. This can be mitigated by connecting a resistor between the bias terminal and V +, raising quiescent current. A feature of the final design is that the output resistance is largely indepen- dent of the follower quiescent current or the output load current. The output will also swing to the negative rail, which is particularly useful with single supply operation. Equivalent Circuit Below 1MHz, the LT1010 is quite accurately represented by the equivalent circuit shown here for both small- and large-signal operation. The internal element, A1, is an ROUT R ′ R ′ R ′= RSAT – ROUT VSOS + V+ V– OUTPUT INPUT IB VOS VSOS – 1010 AI02 + A1 Loaded voltage gain can be determined from the unloaded gain, AV, the output resistance, ROUT, and the load resis- tance, RL, using: A AR RR VL VL OUT L = + Maximum positive output swing is given by: V VV R RR OUT SOS L SAT L + + + = + (– ) The input swing required for this output is: VV R R VV IN OUT OUT L OS OS + + =+ ⎛ ⎝⎜ ⎞ ⎠⎟ + ∆ 1– where ∆VOS is the 100mV clipping specified for the saturation measurements. Negative output swing and input drive requirements are similarly determined. Supply Bypass The buffer is no more sensitive to supply bypassing than slower op amps as far as stability is concerned. The 0.1 µF disc ceramic capacitors usually recommended for op amps are certainly adequate for low frequency work. As always, keeping the capacitor leads short and using a |
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