Note: In case of general purpose OPAMP IC 741, pin 2 is the inverting input and pin 3 is non inverting input
Vin is the input applied at non inverting terminal
From virtual ground concept, voltage at the node of inverting input is also Vin
If we apply KCL at this node we get
Simplifying, we get
As we can see, the given circuits operates as a non inverting
amplifier with a gain of
Here, the as Rf =10k and Ri = 1k, Gain = 11
I have constructed the given circuit on a breadboard in TinkerCAD tool
Both the power supplies used in the circuit are set at 12V, positive terminal of one of the supply goes to the pin 7 of OPAMP IC. Whereas, negative terminal of the other 12V supply goes to the pin 4 of OPAMP. The other two terminals are tied together at ground.
Rest of the components are connected as shown
The input is set at 0.5V/500mV with 10Hz frequency (sine wave)
The output voltage waveform should have the same frequency and a peak to peak amplitude of 0.5*11 = 5.5 V
As can be seen in the simulation, the lower scope shows the input waveform. Y-axis has a span of 1Vp-p.
As input is 500mVp-p, it occupies half the range.
Similarly the y axis span of the scope connected to output is 10Vp-p, so we can see that the output waveform is approximately 5.5Vp-p sine wave in phase with input
Which verifies the calculations above and confirms that the OPAMP is operating as a non inverting amplifier
Inverting Amplifier Figure 4.2 shows the fundamental configuration of Op-Amp in which it is used as an inverting amplifier. In this configuration the ratio, R2/R1 completely controls the effective gain of the amplifier and it can be verified that the output voltage is equal to Vo = - (R2/R1)Vin R2 100K Q-10V R1 Vinow 20K 1 2 7 V Vo 3 -10v Figure 4.2 Part 1 - Inverting Amp: Procedure 1. Construct the circuit of figure 4.2 using Op-Amp IC...
please use multisim
XFG1 xsci Agilent PP 0 0 0 Vin R3 12k0 두 12V XSC2 R1 Voal DD 4.7ko AD741CH R2 122 0 12V 12V Vot HH LM139AJ 120 TO TAG Hot Now, reduce the peak-to-peak voltage of the sawtooth input signal Vin until the fundamental frequency of the output signal V.2 becomes the same as that of the input signal (i.e. 500 Hz). The shape of Voz has to be inverse-sawtooth in this case. Insert below separate images...
LAB TEST 1 (set 1) PMENT REQUIRED 2 Power Supply 3. Function Generator PROCEDURE 1. Connect a circuit as shown in Figure 1 2. Measure the output voltage at Ri. Ra for the given frequency range oscilloscope. Ri 1.6 kW 10 Vpp, 5 kHz 100 nF R 24 KW Figure 1 RESULTS Vpp Vpo at R Freq (kHz) Vou (Vop at Ra) 10 10 03.5t 20 10 30 10 10 50 10 60 70 10 80 10 100 10 ....
thanks
Laboratory 1: operation amplifier characteristics A. Objectives: 1. To study the basic characteristics of an operational amplifier 2. To study the bias circuit of an operational amplifier B. Apparatus: 1. DC Power supply 2. Experimental board and corresponding components 3. Electronic calculator (prepared by students) 4. Digital camera (prepared by students for photo taking of the experimental results) 5. Laptop computer with the software PicoScope 6 and Microsoft Word installed. 6. PicoScope PC Oscilloscope and its accessories. 7. Multimeter...
Ctri Question 3 (20 Marks) Lab 1-Zener Circuits and Applications Theory: Zener diode is designed to operate in reverse conduction. Zener breakdown occurs at a precisely defined voltage, allowing the diode to be used as a voltage reference or clipper. While Zener diodes are usually operated in reverse conduction, they may also be operated in cutoff and forward conduction. There are two different effects that are used in "Zener diodes". The only practical difference is that the two types have...
02 +Vo D3 Rgare 18 Circuit for Problem 1 Analysis 1. Copy the circuit of Figure 1.8 and sketch the ow of pesitive curment throughout the entire circuit for o>0. Repeat for n ce 2. Plot two periods of nlt) and s) for each of the thee input wave shown in Figune 17 on page 37 fom output t (a) Feak value, and b) Eflective DC value, also known as RMS value NotTE These and are therefore optional 4. Determine...