Search This Blog

Kelas 3 Sekolah Dasar

nothing is impossible.

Kelas 9 Sekolah Menengah Pertama

Tabunglah kebajikan, kelak engkau sendiri yang akan menerima kebahagiaan.

Febri,Wancok,Ghani,Ridhwan foto di Braga

Siapa yang menabur kata akan menuai akibat yang baik, memberi berkah yang buruk membawa musibah.

Kelas 3 SMA fotbar di Rumah Saniman

Jangan membenci orang yang mengkritik. Ia adalah guru teori dan praktik sejati bila juga memberi solusi.

Rihlah bareng HKPI

Hidup ini indah, jangan disesali. Nikmati dengan penuh syukur.

Wednesday, March 5, 2014

Instrumentation Amplifier

  • Instrumentation AmplifierOne drawback of the differential amplifier is that its input impedance ($R_3+R_4$) may not be high enough if the output impedance of the previous stage is not low enough. To overcome this problem, two non-inverters with high input resistance can be used each for one of the two inputs to the differential amplifier. The resulting circuit is shown below:
    InstrumentationOpAmp.gif
    The analysis of this circuit is very simple. As the output impedance of the non-inverter is low, the three op-amp circuit can be considered as three independent circuits. The outputs of the two non-inverters are:

    \begin{displaymath}V'_1=V_1\left(1+\frac{R_f}{R_1}\right),\;\;\;\;\;\;\;\;\;
V'_2=V_2\left(1+\frac{R_f}{R_1}\right) \end{displaymath}


    The output voltage of the differential amplifier is:

    \begin{displaymath}V_{out}=\frac{R_4}{R_3}(V'_2-V'_1)=\frac{R_4}{R_3}\left(1+\frac{R_f}{R_1}\right)(V_2-V_1) \end{displaymath}


    Of course the two resistors $R_1$ can be combined to become $R_0=2R_1$, i.e., $R_1=R_0/2$, then the output can be written as:

    \begin{displaymath}V_{out}=\frac{R_4}{R_3}\left(1+\frac{2R_f}{R_0}\right)(V_2-V_1) \end{displaymath}


    Alternatively, we consider the current going from $V'_1$ to $V_'_2$:

    \begin{displaymath}\frac{V'_1-V_1}{R_f}=\frac{V_1-V_0}{R_1}=\frac{V_0-V_2}{R_1}=\frac{V_2-V'_2}{R_f} \end{displaymath}


    From the equation of the first two terms we get:

    \begin{displaymath}V'_1=\left(1+\frac{R_f}{R_1}\right)V_1-\frac{R_f}{R_1}V_0 \end{displaymath}


    From the equation of the second two terms we get:

    InstrumentationOpAmp.gif$R_3+R_4$\begin{displaymath}V'_2=\left(1+\frac{R_f}{R_1}\right)V_2-\frac{R_f}{R_1}V_0 \end{displaymath}


    Using the equation of the differential amplifier above, we get the same result as above:

    \begin{displaymath}V_{out}=\frac{R_4}{R_3}(V'_2-V'_1)=\frac{R_4}{R_3}\left(1+\frac{R_f}{R_1}\right)(V_2-V_1) \end{displaymath}






sumber : http://fourier.eng.hmc.edu/e84/lectures/opamp/node3.html

Jadwal Semester II


Hari / JamMata Kuliah
SeninNama
7.00 - 7.50T
7.50 - 8.40ElektronikaT
8.40 - 9.30ElektronikaT
9.30 - 10.20ElektronikaT
10.40 - 11.30Kimia TerapanT
11.30 - 12.20Kimia TerapanT
13.00 - 13.50Kimia TerapanP
13.50 - 14.40Kimia TerapanP
14.40 - 15.30Kimia TerapanP
15.50 - 16.40Kimia TerapanP
16.40 - 17.30
17.30 - 18.20
Selasa
7.00 - 7.50Bahasa IndonesiaT
7.50 - 8.40Bahasa IndonesiaT
8.40 - 9.30Bahasa IndonesiaT
9.30 - 10.20ElektronikaP
10.40 - 11.30ElektronikaP
11.30 - 12.20ElektronikaP
13.00 - 13.50ElektronikaP
13.50 - 14.40
14.40 - 15.30Mekanika TeknikT
15.50 - 16.40Mekanika TeknikT
16.40 - 17.30
17.30 - 18.20
Rabu
7.00 - 7.50Matematika Terapan IIT
7.50 - 8.40Matematika Terapan IIT
8.40 - 9.30Matematika Terapan IIT
9.30 - 10.20
10.40 - 11.30Gambar Teknik IIP
11.30 - 12.20Gambar Teknik IIP
13.00 - 13.50Gambar Teknik IIP
13.50 - 14.40Gambar Teknik IIP
14.40 - 15.30Gambar Teknik IIP
15.50 - 16.40
16.40 - 17.30
17.30 - 18.20
Kamis
7.00 - 7.50Termodinamika TeknikT
7.50 - 8.40Termodinamika TeknikT
8.40 - 9.30Termodinamika TeknikT
9.30 - 10.20
10.40 - 11.30
11.30 - 12.20Instrumentasi dan PengukuranP
13.00 - 13.50Instrumentasi dan PengukuranP
13.50 - 14.40Instrumentasi dan PengukuranP
14.40 - 15.30Instrumentasi dan PengukuranP
15.50 - 16.40Instrumentasi dan PengukuranP
16.40 - 17.30Instrumentasi dan PengukuranP
17.30 - 18.20
Jumat
7.00 - 7.50
7.50 - 8.40
8.40 - 9.30
9.30 - 10.20
10.20 - 11.10
11.10 - 12.40
12.40 - 13.30
13.30 - 14.20
14.20 - 15.10
15.30 - 16.20
16.20 - 17.10
17.10 - 18.00