| поискавой системы для электроныых деталей |
|
LMV716 датащи(PDF) 11 Page - National Semiconductor (TI) |
|
|
|
|||||||||||||||||||||||||||||
LMV716 датащи(HTML) 11 Page - National Semiconductor (TI) |
|
11 / 15 page ![]() Application Information (Continued) Now looking at the output of the instrumentation amplifier: (5) Substituting from Equation (4): (6) This shows the gain of the instrumentation amplifier to be: −K(2a+1) Typical values for this circuit can be obtained by setting: a = 12 andK=4. This results in an overall gain of −100. Three LMV716 amplifiers are used along with 1% resistors to minimize resistor mismatch. Resistors used to build the circuit are: R 1 = 21.6 k Ω,R 11 = 1.8 k Ω,R 2 = 2.5 k Ω with K = 40 and a = 12. This results in an overall gain of −K(2a+1) = −1000. Two-Op-Amp Instrumentation Amplifier A two-op-amp instrumentation amplifier can also be used to make a high-input impedance DC differential amplifier Figure 6). As in the three op amp circuit, this instrumentation am- plifier requires precise resistor matching for good CMRR. R 4 should be equal to R 1, and R3 should equal R2. ACTIVE FILTERS Active filters are circuits with amplifiers, resistors, and ca- pacitors. The use of amplifiers instead of inductors, which are used in passive filters, enhances the circuit performance while reducing the size and complexity of the filter. The simplest active filters are designed using an inverting op amp configuration where at least one reactive element has been added to the configuration. This means that the op amp will provide "frequency-dependent" amplification, since reac- tive elements are frequency dependent devices. Low Pass Filter The following shows a very simple low pass filter. The transfer function can be expressed as follows: By KCL: (7) Simplifying this further results in: (8) or (9) Now, substituting ω=2πf, so that the calculations are in f(Hz) rather than in ω(rad/s), and setting the DC gain and (10) set: (11) Low pass filters are known as lossy integrators because they only behave as integrators at higher frequencies. The gen- eral form of the bode plot can be predicted just by looking at the transfer function. When the f/f O ratio is small, the capaci- tor is, in effect, an open circuit and the amplifier behaves at a set DC gain. Starting at f O, which is the −3 dB corner, the capacitor will have the dominant impedance and hence the circuit will behave as an integrator and the signal will be attenuated and eventually cut. The bode plot for this filter is shown in Figure 8. 20179513 FIGURE 6. Two-Op-Amp Instrumentation Amplifier 20179553 FIGURE 7. Low Pass Filter www.national.com 11 |
|
|
ссылки URL |
| Вашему бизинису помогли Аллдатащит? [ DONATE ] |
Что такое Аллдатащит | реклама | контакт | Конфиденциальность | Ссылка на техническое описание | обмен ссыками | поиск по производителю All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |