V}{{{V_T}}}}}\)By APPLYING KCL at NODE O,\(I = \frac{{0 - {V_{out}}}}{{1k}} = {I_o}{e^{\frac{{{V_{in}}}}{{{V_T}}}}}\)\(\Rightarrow {V_{out}} \propto {e^{\frac{{{V_{in}}}}{{{V_T}}}}}\)

"> V}{{{V_T}}}}}\)By APPLYING KCL at NODE O,\(I = \frac{{0 - {V_{out}}}}{{1k}} = {I_o}{e^{\frac{{{V_{in}}}}{{{V_T}}}}}\)\(\Rightarrow {V_{out}} \propto {e^{\frac{{{V_{in}}}}{{{V_T}}}}}\)

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In the circuit shown below, the input voltage Vin in positive. The current (I) - voltage (V) characteristics of the diode can be assumed to be I = I0­eV/VT under the forward bias condition, where VT is the thermal voltage and I0 is the reverse saturation current. Assuming an ideal op-amp, the output voltage Vout of the circuit is proportional to

Electronics & Communication Engineering Op-Amp And Its Applications in Electronics & Communication Engineering . 7 months ago

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\(I = {I_o}{e^{\frac{V}{{{V_T}}}}}\)By APPLYING KCL at NODE O,\(I = \frac{{0 - {V_{out}}}}{{1k}} = {I_o}{e^{\frac{{{V_{in}}}}{{{V_T}}}}}\)\(\Rightarrow {V_{out}} \propto {e^{\frac{{{V_{in}}}}{{{V_T}}}}}\)

Posted on 27 Oct 2024, this text provides information on Electronics & Communication Engineering related to Op-Amp And Its Applications in Electronics & Communication Engineering. Please note that while accuracy is prioritized, the data presented might not be entirely correct or up-to-date. This information is offered for general knowledge and informational purposes only, and should not be considered as a substitute for professional advice.

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