{"id":2818,"date":"2024-08-23T03:59:57","date_gmt":"2024-08-22T20:59:57","guid":{"rendered":"https:\/\/www.tneutron.net\/elektro\/?p=2818"},"modified":"2024-08-21T07:48:19","modified_gmt":"2024-08-21T00:48:19","slug":"strengthening-open-loop-op-amp","status":"publish","type":"post","link":"https:\/\/www.tneutron.net\/elektro\/strengthening-open-loop-op-amp\/","title":{"rendered":"Strengthening Open-Loop Op-Amp"},"content":{"rendered":"<p><span class=\"notranslate\">The op-amp ideally has an infinite open-loop gain (AOL).<\/span> <span class=\"notranslate\"> In practice, however, op-amps such as LM741 have a finite amplification of approximately 100,000 times.<\/span> <span class=\"notranslate\"> Actually with this bigger gain, the op-amp gain system becomes unstable.<\/span> <span class=\"notranslate\"> Very small differential inputs can already make the outputs a manifestation.<\/span> <span class=\"notranslate\"> In the next chapter will discuss how feedback can make the op-amp&#8217;s reinforcement system stabilized.<\/span><\/p>\n<p><span class=\"notranslate\"> <strong>A. Unity-Gain Frequency<\/strong><\/span><br \/>\n<span class=\"notranslate\"> The ideal Op-Amp should work at any frequency ranging from dc signal to Herzt giga frequency.<\/span> <span class=\"notranslate\"> Unity-gain frequency parameter becomes important if the op-amp is used for certain frequency applications.<\/span> <span class=\"notranslate\"> Parameter AOL is usually a gain of op-amp on DC signal.<\/span><\/p>\n<p><span class=\"notranslate\"> Response of op-amp gain decreases as the input signal frequency increases.<\/span> <span class=\"notranslate\"> Op-amp LM741 for example has unity-gain frequency of 1MHz.<\/span> <span class=\"notranslate\"> This means the amplification of the op-amp will be 1 time at 1 MHz frequency.<\/span> <span class=\"notranslate\"> If you need to design the application at high frequency, then choose op-amp that has higher unity-gain frequency.<\/span><\/p>\n<p><span class=\"notranslate\"> <strong>B. Op-Amp Ideal<\/strong><\/span><br \/>\n<span class=\"notranslate\"> Op-Amp is basically a differential amplifier that has two inputs.<\/span> <span class=\"notranslate\"> Input (input) op-amps as already understandable there are so-called inverting and non-inverting inputs.<\/span> <span class=\"notranslate\"> The deal op-amp has an infinite open loop gain.<\/span> <span class=\"notranslate\"> Like the LM741 op-amp often used by many electronics practitioners, it has the typical characteristics of an open loop gain of 10 <sup>4<\/sup> ~ 10 <sup>5 This<\/sup> magnitude gain makes the op-amp unstable, and its gain becomes infinite.<\/span><\/p>\n<p><span class=\"notranslate\"> This is where the role of the negative feedback circuit is required, so that the op-amp can be assembled into an application with a measured value of finite.<\/span> <span class=\"notranslate\"> The ideal op-amp input impedation should be infinite, so that the input current at each input should be 0. As a practical comparison, the LM741 op-amp has an input impedance Z <sub>in<\/sub> = 10 <sup>6<\/sup> Ohm.<\/span> <span class=\"notranslate\"> The impedance value is still relatively large so the input current of the LM741 op-amp should be very small.<\/span><\/p>\n<p><span class=\"notranslate\"> There are two important rules for analyzing op-amp circuits based on ideal op-amp characteristics.<\/span> <span class=\"notranslate\"> This rule in some literature is called golden rule, namely:<\/span><br \/>\n<a href=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2017\/05\/clip_image002.jpg\"><img loading=\"lazy\" decoding=\"async\" title=\"Clip_image002\" src=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2017\/05\/clip_image002_thumb.jpg\" alt=\"clip_image002\" width=\"304\" height=\"58\" border=\"0\" \/><\/a><br \/>\n<span class=\"notranslate\"> <b><i>These are two important rules of ideal op-amps used to analyze op-amp circuits.<\/i><\/b><\/span><\/p>\n<p><span class=\"notranslate\"> <b>C. Inverting Amplifier<\/b><\/span><br \/>\n<span class=\"notranslate\"> The inverting amplifier base circuit as shown in Figure 1, where the input signal is generated through the inverting input.<\/span> <span class=\"notranslate\"> As the name implies, the reader would have guessed that the output phase of this inverting amplifier would always be in reverse with the input.<\/span> <span class=\"notranslate\"> In this circuit, negative feedback is generated through resistor R2.<\/span><br \/>\n<a href=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2017\/05\/clip_image0021.jpg\"><img loading=\"lazy\" decoding=\"async\" title=\"Clip_image002 [1]\" src=\"https:\/\/www.tneutron.net\/elektro\/wp-content\/uploads\/sites\/2\/2017\/05\/clip_image0021_thumb.jpg\" alt=\"clip_image002[1]\" width=\"274\" height=\"194\" border=\"0\" \/><\/a><br \/>\n<span class=\"notranslate\"> Inverter Drawer Image<\/span><\/p>\n<p><span class=\"notranslate\"> The non-inverting input in the circuit is grounded, or v <sub>+<\/sub> = 0. With rule 1 (see rule 1), it will be dipenuhiv <sub>&#8211;<\/sub> = v <sub>+<\/sub> = 0. Since the value is 0 but not directly connected to ground, the op-amp- In this circuit is called virtual ground.<\/span> <span class=\"notranslate\"> With this fact, it can be calculated the clamp voltage at R1 is v <sub>in<\/sub> -v = vin and the clamp voltage of the reactor R2 is v <sub>out<\/sub> -v <sub>&#8211;<\/sub> = v <sub>out<\/sub> Then by using rule 2, it is known that: i <sub>in<\/sub> + i <sub>out<\/sub> = I = 0, Because according to rule 2, the input current of the op-amp is 0 i <sub>in<\/sub> + i <sub>ou<\/sub> t = v <sub>in<\/sub> \/ R <sub>1<\/sub> + v <sub>out<\/sub> \/ R <sub>2<\/sub> = 0 Next vout \/ R2 = -v <sub>in<\/sub> \/ R1 or v <sub>out<\/sub> \/ v <sub>in<\/sub> = -R2 \/ R1<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"<p>The op-amp ideally has an infinite open-loop gain (AOL). In practice, however, op-amps such as LM741 have a finite amplification<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"colormag_page_container_layout":"default_layout","colormag_page_sidebar_layout":"default_layout","footnotes":""},"categories":[2232],"tags":[3486,3488,3482,3483,3481,3489,3485,3487,3484,3480],"class_list":["post-2818","post","type-post","status-publish","format-standard","hentry","category-english","tag-open-loop-op-amp-calculator","tag-open-loop-op-amp-characteristics","tag-open-loop-op-amp-circuit","tag-open-loop-op-amp-comparator","tag-open-loop-op-amp-configuration","tag-open-loop-op-amp-configuration-pdf","tag-open-loop-op-amp-example","tag-open-loop-op-amp-gain-at-10-khz","tag-open-loop-op-amp-saturation","tag-open-loop-op-amp"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.9 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Strengthening Open-Loop Op-Amp - TN Elektro<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.tneutron.net\/elektro\/strengthening-open-loop-op-amp\/\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:title\" content=\"Strengthening Open-Loop Op-Amp - TN Elektro\" \/>\n<meta name=\"twitter:description\" content=\"The op-amp ideally has an infinite open-loop gain (AOL). 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