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LT1251CS Datasheet(PDF) 13 Page - Linear Technology |
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LT1251CS Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() 13 LT1251/LT1256 APPLICATIONS INFORMATION In low gain applications, R1 and R2 are small compared to the feedback resistors and therefore we can simplify the equation to: V KV RR RR KV RR RR sR C R K R K R O GF GF GF GF OL OL F F = ()( ) + + − () ()( ) + + ++ − () 1 11 11 2 22 22 12 1 1 1 Note that the denominator causes a gain error due to the open-loop gain (typically 0.1% for frequencies below 20kHz) and for mismatches in RF1 and RF2. A 1% mis- match in the feedback resistors results in a 0.25% error at K = 0.5. If we set RF1 = RF2 and assume ROL >> RF1 (a 0.1% error at low frequencies) the above equation simplifies to: and VKV A K V A where A R R A R R OV V V F G V F G =+ − () =+ =+ 11 2 2 1 1 1 2 2 2 1 11 This shows that the output fades linearly from input 2, times its gain, to input 1, times its gain, as K goes from 0 to 1. If only one input is used (for example, V1) and Pin 14 is grounded, then the gain is proportional to K. V V KA O V 1 1 = Similarly for the inverting case where the noninverting inputs are grounded and the input voltages V1 and V2 drive the normally grounded ends of RG1 and RG2, we get: General Equation for the Inverting Amplifier Case V KV RR R R KV RR R R sR C R K RR R R K RR R R O G G F G G F OL OL F F G F F G =− ++ + − () ++ + + ++ + − () ++ 1 11 1 1 2 22 2 2 11 1 1 22 2 2 1 1 1 1 1 1 1 Note that the denominator is the same as the noninverting case. In low gain applications, R1 and R2 are small compared to the feedback resistors and therefore we can simplify the equation to: V KV R KV R sR C R K R K R O GG OL OL F F =− + − () + ++ − () 1 1 2 2 12 1 1 1 Again, if we set RF1 = RF2 and assume ROL >> RF1 (a 0.1% error at low frequencies) the above equation simplifies to: and VKV A K V A where A R R A R R OV V V F G V F G =− + − () [] == 11 2 2 1 1 1 2 2 2 1 The 4-resistor difference amplifier yields the same result as the inverting amplifier case, and the common mode rejection is independent of K. |
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