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Let's look at simple reverse polarity protection circuits using diodes.<\/strong><\/p>\n\n<h2 id=\"reverse-polarity-protecti\">Reverse Polarity Protection<a href=\"#reverse-polarity-protecti\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>The right polarity matters. Almost all semiconductor components and electrolytic capacitors are sensitive in regard to reverse voltages. Applying a reverse voltage, even by accident and for a short time, can easily destroy devices. In this article, we will look at simple reverse polarity protection circuits using just a diode.<\/p>\n<p>There are two different ways how to place the diode in such a protection circuit:<\/p>\n<ol>\n<li>Putting a diode in series to the load<\/li>\n<li>Using a diode as a shunt in parallel to the load<\/li>\n<\/ol>\n<p><img loading=\"lazy\" alt=\"Reverse polarity protection with diodes\" src=\"\/user\/pages\/02.blog\/reverse-polarity-protection\/diode-reverse-polarity-protection.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>Let's have a deeper look at these two options and their advantages and disadvantages.<\/p>\n<h2 id=\"diode-in-series\">Diode in Series<a href=\"#diode-in-series\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>The most common reverse polarity protection circuit is to connect a diode in series to the circuit. If reverse biased, the diode blocks the current flow and by that protects the attached circuit.<\/p>\n<p>An example for this is the protection circuit for the Arduino Uno's barrel jack connector. As shown in the picture below there is a diode right next to the connector. This diode provides protection, in case a reverse voltage is supplied via the barrel jack.<\/p>\n<p><img loading=\"lazy\" alt=\"Reverse polarity protection diode next to the barrel jack connector of the Arduino\" src=\"\/user\/pages\/02.blog\/reverse-polarity-protection\/arduino-protection-diode.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>Link: <a href=\"https:\/\/content.arduino.cc\/assets\/UNO-TH_Rev3e_sch.pdf\">Arduino Schematic<\/a><\/p>\n<h2 id=\"diode-as-shunt\">Diode as Shunt<a href=\"#diode-as-shunt\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Alternatively, a diode can be used as shunt. A shunt is an alternative low-ohmic current path. On this path, the current can pass around the protected circuit in case of reverse polarity.<\/p>\n<p>For diodes and LEDs a typical example for this is a so-called antiparallel diode. As you can see in the circuit diagram below, the diode is added in the reverse direction of the LED.\n<img loading=\"lazy\" alt=\"Reverse polarity protection with an anti-parallel diode\" src=\"\/user\/pages\/02.blog\/reverse-polarity-protection\/diode-anti-parallel.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>Under normal conditions the protection diode is reverse biased and the current flows through the LED. In case of a reverse voltage the diode becomes conductive and the current flows through it instead. The LED is protected. <\/p>\n<h2 id=\"from-theory-to-practice\">From Theory to Practice<a href=\"#from-theory-to-practice\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>In theory, the in-series diode is the optimal reverse voltage protection. It seems like a simple, but effective measure to block any reverse current flow.\nHowever, it is the practice that matters. In practice, there is no ideal solution. Why, you ask?\nBecause in practice diodes are far from perfect:<\/p>\n<ol>\n<li><strong>Diodes are no perfect conductors in forward direction<\/strong><br>\nThe forward voltage drop is the measure that quantifies the diode's deficiency in regard to being a perfect conductor in forward direction.\nFor standard silicon diodes it is around 0.7 V and for schottky diodes around 0.3\nV.<\/li>\n<li><strong>Diodes are no perfect isolators in reverse direction<\/strong><br>\nThe reverse leakage current characterizes how well the diode can suppress any reverse current flow. A standard diode has a leakage current of a few microamperes. Schottky diodes have significantly more leakage current in the area of several milliamperes.<\/li>\n<\/ol>\n<h3 id=\"consequences-for-an-in-se\">Consequences for an in-series diode<a href=\"#consequences-for-an-in-se\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h3>\n<p>Whenever you put a diode in series to a circuit, the supply voltage will be lowered by the diodes forward voltage drop. The lost energy will be dissipated as heat produced within the diode.\nIn consequence an in-series is...<\/p>","tags":["electronics","diodes"],"image":"\/user\/pages\/02.blog\/reverse-polarity-protection\/reverse-protection-diode.jpg?g-982d5237"},{"title":"Photoelectric Effect","date_published":"2023-09-18T08:00:00+02:00","id":"https:\/\/devxplained.eu\/en\/blog\/photoelectric-effect","url":"https:\/\/devxplained.eu\/en\/blog\/photoelectric-effect","content_html":"<p><strong>Electromagnetic radiation, like light, interacts with electrons. This is called the photoelectric effect.<\/strong><\/p>\n\n<h2 id=\"photoelectric-effect\">Photoelectric Effect<a href=\"#photoelectric-effect\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Light interacts with matter. If a photon with an high enough energy hits an electron, it can knock it out of its place. This leaves a free electron and an electron hole behind. This light-matter interaction is what is known as the photoelectric effect.<\/p>\n<p>In today's article, we are going to look at three different physical phenomenons that are caused by or can be subsumed under the photoelectric effect. This will give us the necessary background knowledge for understanding photoelectric components like light dependent resistors, photodiodes and solar cells.<\/p>\n<p><img loading=\"lazy\" alt=\"The photoelectric effect: Photons can excite electrons generating electron-hole pairs\" src=\"\/user\/pages\/02.blog\/photoelectric-effect\/photoelectric-effect-bohr-model.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<h3 id=\"photoelectric-emission\">Photoelectric Emission<a href=\"#photoelectric-emission\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h3>\n<p>Let's start with photoelectric emission which is also called Hallwachs effect. It is the phenomenon, that has lead to the discovery and understanding of the photoelectric effect. Thus, if you search for photoelectric effect, you typically find this effect. However, while this effect is scientifically of utmost importance, it has almost no relevancy in the context of electronics. It's worth having a look anyway, for having better understanding of the photoelectric effect and its properties.<\/p>\n<p>Heinrich Hertz is a German physicist famous for his research on electromagnetic waves. In one of his experiments he noticed that the results differed if his setup was put in a glass box. He discovered, that using quartz instead of glass solved the issue as quartz does not filter out the UV light as glass does. In 1887, he did further experiments on this phenomenon and described it. The physicist Willhelm Hallwachs later continued them. He came up with the following setup:<\/p>\n<p><img loading=\"lazy\" alt=\"Hallwachs' experiment: a charged zinc plate is put on an electroscope and illuminated\" src=\"\/user\/pages\/02.blog\/photoelectric-effect\/hallwachs-experimental-setup.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>A zinc plate is placed on top of a gold-leaf electroscope. If  charged up, the fine bend gold-leaf attached in center get too. Since its two ends have the same polarity, they repel each other and the gold-leaf opens up.<\/p>\n<p><img loading=\"lazy\" alt=\"Hallwachs effect\" src=\"\/user\/pages\/02.blog\/photoelectric-effect\/hallwachs-effect.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>Hallwachs charged up the zinc plate negatively and discovered, that if the UV-light hits the zinc plate, it slowly discharges. He repeated his experiments with different configurations and found out, that even if the zinc plate is initially uncharged, it will slowly become more and more positively charged.\nHis conclusion was that zinc emits negative charge carriers when exposed to UV-light.<\/p>\n<p><img loading=\"lazy\" alt=\"Photoelectric emission describes the emission of electrons from a material under the influence of light\" src=\"\/user\/pages\/02.blog\/photoelectric-effect\/photoemission.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>He ought to be right. When the UV-light hits the zinc surface electrons are emitted from it. Nowadays, this is what is known as photoelectric emission or often simply the photoelectric effect.\nHowever, this seemingly simple phenomenon posed loads of new questions to the scientific community. Why does it have to be UV-light? Why does the energy of the emitted electrons not depend on the light intensity, but the wavelength? <\/p>\n<p>Notable scientists like Max Planck and Albert Einstein helped to answer these questions during next century. Their answers turned the existing knowledge about electromagnetic waves upside down and took part in the development of quantum physics.<\/p>\n<p>Important for us is, that light has both wave and particle properties. The photoelectric effect is easiest to understand, when describing light as particles called photons. The energy of these...<\/p>","tags":["electronics","physics","diodes","light"],"image":"\/user\/pages\/02.blog\/photoelectric-effect\/photoelectric-effect.jpg?g-982d5237"},{"title":"TVS Diodes","date_published":"2023-05-08T08:00:00+02:00","id":"https:\/\/devxplained.eu\/en\/blog\/tvs-diodes","url":"https:\/\/devxplained.eu\/en\/blog\/tvs-diodes","content_html":"<p><strong>TVS diodes protect circuits from voltage spikes. Let's discover what they are and what makes them special!<\/strong><\/p>\n\n<h2 id=\"tvs-diodes\">TVS Diodes<a href=\"#tvs-diodes\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Transient voltage suppressor (TVS) diodes are a type of diodes, that is specifically designed to protect circuits. To use it, connect the TVS diode reverse biased in parallel to the circuit.\n<img loading=\"lazy\" alt=\"TVS diode used to protect a circuit\" src=\"\/user\/pages\/02.blog\/tvs-diodes\/tvs-circuit.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>The circuit seems to be identical to the one used for voltage regulation or voltage references using a zener diode. Technically, this is true. This is the circuit of a <a href=\"\/en\/blog\/zener-diodes-as-shunt-regulator\">shunt regulator<\/a>. However, it is used differently. To protect a 5 V circuit one chooses a TVS diode that starts to conduct slightly above 5 V.\nA TVS diode is intended as overvoltage protection and not as voltage regulator. As the name implies, it suppresses voltage transients by absorbing them.<\/p>\n<div class=\"notices blue\">\n<p><strong>What Are Transients?<\/strong><br>\nA transient, voltage spike or power surge is a sudden, short time, release of electrical energy. For a short time the voltage can rise high above the usual operating voltage of the circuit. This has the potential to destroy a circuit. Typical, sources for voltage transients are electrostatic discharge (ESD), lightning strikes, the switching of inductive loads or the turn-on overshoot of switch mode power supplies.<\/p>\n<\/div>\n<p>TVS diodes are zener diodes, however, they are special zener diodes. A TVS diode can absorb huge amounts of power. Small zener diodes are usually rated for 0.5 W, TVS diodes can handle several hundred watts and often more than a kilowatt for a very short amount of time without getting damaged. For a short amount of time is the important keyword here. A short amount of time, is all that is needed to prevent a voltage transient from damaging a circuit. However, TVS diodes are not intended for permanent loads. <\/p>\n<p>What is a short amount of time? That is specified in the datasheet of each diode. What is essential to understand is, that values like the peak pulse power rating of TVS diodes are measured according to industry-standards like the IEC61643-123 (10\/1000 &micro;s waveform). These standards make certain assumptions about the voltage transients. The 10\/1000 &micro;s waveform for example tries to resemble short, but high power, transients as they occur in case of lightning strikes or ESD. Voltage transients caused by inductive loads often last longer. In such a case, a TVS diode needs to be derated.<\/p>\n<p>As TVS diode can absorb such high amounts of power, it is not required to add a current limiting resistor in series. The source and wire impedance is usually high enough. No power has to wasted by an additional current limiting resistor. <\/p>\n<p>The schematic symbol for TVS diodes is identical to the one used for zener diodes. However, if used correctly, there are two type of TVS diodes to differentiate between: unidirectional and bidirectional TVS diodes.\n<img loading=\"lazy\" alt=\"Schematic symbol for uni- and bidirectional TVS diodes\" src=\"\/user\/pages\/02.blog\/tvs-diodes\/tvs-diodes.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>Unidirectional TVS diodes are for DC circuits. If forward-biased they conduct at roughly 0.7 V like normal diodes. Their voltage rating only applies when they are reverse biased.<\/p>\n<p>Bidirectional TVS diodes are for AC circuits where...<\/p>","tags":["electronics","diodes"],"image":"\/user\/pages\/02.blog\/tvs-diodes\/tvs-diodes.jpg?g-982d5237"},{"title":"Zener Diodes as Shunt Regulator","date_published":"2023-04-17T08:00:00+02:00","id":"https:\/\/devxplained.eu\/en\/blog\/zener-diodes-as-shunt-regulator","url":"https:\/\/devxplained.eu\/en\/blog\/zener-diodes-as-shunt-regulator","content_html":"<p><strong>Building a voltage source for small circuits with a zener diode? Let's explore how this is possible, let's build a shunt regulator.<\/strong><\/p>\n\n<h2 id=\"zener-diodes-as-shunt-reg\">Zener Diodes as Shunt Regulator<a href=\"#zener-diodes-as-shunt-reg\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>You have developed a small circuit, but the voltage it is designed for is not available in the target environment? This not an uncommon situation. The 5 V or 3.3 V that are used in many microcontroller circuits are not used everywhere. <\/p>\n<p>What do you do in such a case? You need a voltage regulator. A voltage regulator is a circuit that provides your circuit with the constant voltage you require.\nToday, we are going to look at a very simple voltage regulator circuit: a shunt regulator. We can build it using just a zener diode and a resistor. Let's have a look!<\/p>\n<h2 id=\"what-is-a-shunt-regulator\">What is a Shunt Regulator?<a href=\"#what-is-a-shunt-regulator\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>When talking about voltage regulators there are two main types to differentiate between: linear regulators and switch mode regulators. Switch mode regulators are efficient, but complicated to build. They use a switching element like a transistor or MOSFET to regulate the voltage and can both reduce the input voltage, this is called a buck converter, or increase it, which is called a boost converter. Linear regulators can only reduce the input voltage.<\/p>\n<p>There are two types of linear regulators, a shunt regulator is one them and at the same time one of the simplest voltage regulator circuits. Shunt regulators as opposed to in series linear regulators, regulate the voltage by providing a current path in parallel to the load through which they sink the surplus current.<\/p>\n<p><img loading=\"lazy\" alt=\"Shunt regulator based on a zener diode\" src=\"\/user\/pages\/02.blog\/zener-diodes-as-shunt-regulator\/zener-as-shunt-regulator.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>For a shunt regulator to work the overall current has to be limited. This is typically achieved by connecting a resistor in series to the circuit. The core component of the regulator is, however, the actual regulating element, also called control element. This is the component that ensures the constant output voltage. For that, it not only provides the alternative current path, but more importantly, controls how much current needs flows through it so that the voltage remains constant. In our circuit, this is achieved using a zener diode. It limits the output voltage to its zener voltage and sinks the remaining current.<\/p>\n<div class=\"notices blue\">\n<p><strong>Does the circuit look familiar to you?<\/strong><br>\nIt's practically identical to the one used when using a <a href=\"\/en\/blog\/zener-diodes-as-voltage-reference\">zener diode as voltage reference<\/a>.\nVoltage references are one of the most common applications of shunt regulators. However, if we want to power a small circuit the current limiting resistor has to be chosen much smaller than for a voltage reference.<\/p>\n<\/div>\n<h2 id=\"an-example-circuit\">An Example Circuit<a href=\"#an-example-circuit\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Let's have a look at an example circuit. The shunt regulator in the example powers a small microcontroller, an ATtiny85. The ATtiny85 normally operates at 5V. The shunt regulator circuit allows us to use it with 9 V or 12 V batteries. It achieves this with the help of a simple 5.1V zener diode.<\/p>\n<div class=\"tabs-wrapper ui-theme-default top-left\">\n    <ul class=\"tabs-nav\">\n                    <li class=\"current\"><a href=\"#990c9e40f80\" id=\"Tab0\" rel=\"tab\">Breadboard<\/a><\/li>\n                    <li><a href=\"#990c9e40f81\" id=\"Tab1\" rel=\"tab\">Schematic<\/a><\/li>\n        <\/ul>\n    <div class=\"tabs\">\n            <div class=\"tab\" id=\"990c9e40f80\" style=\"display: block\">\n<p><img loading=\"lazy\" alt=\"Shunt regulator circuit built on a breadboard\" src=\"\/user\/pages\/02.blog\/zener-diodes-as-shunt-regulator\/attiny-shunt-regulator-Breadboard.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<\/div>\n            <div class=\"tab\" id=\"990c9e40f81\" style=\"display: none\">\n<p><img loading=\"lazy\" alt=\"Schematic for the shunt regulator circuit\" src=\"\/user\/pages\/02.blog\/zener-diodes-as-shunt-regulator\/attiny-shunt-regulator-Circuit.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<\/div>\n        <\/div>\n<\/div>\n\n<p>The ATtiny85 runs a small program, that lets the connected LED blink. However, this is not the focus...<\/p>","tags":["electronics","diodes"],"image":"\/user\/pages\/02.blog\/zener-diodes-as-shunt-regulator\/zener-diodes-as-shunt-regulator.jpg?g-982d5237"},{"title":"Zener Diode Low Voltage Alarm","date_published":"2023-03-13T08:00:00+01:00","id":"https:\/\/devxplained.eu\/en\/blog\/zener-diode-low-voltage-alarm","url":"https:\/\/devxplained.eu\/en\/blog\/zener-diode-low-voltage-alarm","content_html":"<p><strong>Today, we are going to build a low voltage alarm using a zener diode and an LM393 comparator.<\/strong><\/p>\n\n<h2 id=\"low-voltage-alarm-with-a-\">Low Voltage Alarm with a Zener Diode<a href=\"#low-voltage-alarm-with-a-\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Last time, we looked at how a zener diode can be used as a voltage reference. This time, we are going to look at a more practical example. We are going to build a low voltage alarm for a 12 V lead acid battery using a zener diode and a comparator.<\/p>\n<p>Let's have a look at what we are trying to achieve: we want an LED or a buzzer to turn on as soon as the battery voltage drops below a certain level. For that we have to define a suitable threshold value. <\/p>\n<p>For a 12 V AGM lead acid battery, 12 V is a good value. That might seem surprising at first, but a modern 12 V AGM lead acid battery gets charged with 14.7 V and should have a voltage of roughly 13 V when fully charged. Additionally, it should not be discharged below 50 % of its capacity, if you want it to last for a long time. These 50 % happen to be reached at 12 V.<\/p>\n<p>Enough theory. Let's build the circuit.<\/p>\n<h2 id=\"the-circuit\">The Circuit<a href=\"#the-circuit\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>For the circuit we again use the LM393 comparator. A comparator compares the voltages at its two inputs. In case the voltage at its non-inverting input (<code>+<\/code>) is lower than the one at the inverting input (<code>-<\/code>), its output becomes low and the LED turns on.<\/p>\n<p>In the circuit I used a 9 V zener diode as a voltage reference and connected it to the LM393's inverting input.  <\/p>\n<div class=\"notices blue\">\n<p><strong>Why 9 V and not 12 V?<\/strong><br>\nIf the battery voltage drops below 12 V the zener won't magically keep the voltage at the inverting input at 12 V. The zener can only reduce the voltage and not increase it. For reacting on the battery voltage falling below 12 V, our voltage reference needs to be stable below 12 V, as well.<\/p>\n<p><strong>Why not 5 V or 3.3 V?<\/strong><br>\nAs discussed last time, we need an avalanche diode and not a real zener for building a stable voltage reference. Below 5 V the zener effect becomes the dominating breakdown effect.<\/p>\n<\/div>\n<p>How does that match our goal to turn the LED on at a battery voltage of 12 V?<br>\nFor measuring the battery voltage, we are going to use a voltage divider. We need to choose the resistor values so that at 12 V the voltage divider outputs 9 V.\nThis can be achieved by using a 3.3 k&Omega; and a 10 k&Omega; resistor. If you want to know more on how to calculate these values, I recommend you to have a look at my article about <a href=\"\/en\/blog\/voltage-dividers#resistor-calculator\">voltage dividers<\/a>.<\/p>\n<p>This is how the finished circuit looks like:<\/p>\n<div class=\"tabs-wrapper ui-theme-default top-left\">\n    <ul class=\"tabs-nav\">\n                    <li class=\"current\"><a href=\"#c78ece9e2b0\" id=\"Tab0\" rel=\"tab\">Breadboard<\/a><\/li>\n                    <li><a href=\"#c78ece9e2b1\" id=\"Tab1\" rel=\"tab\">Schematic<\/a><\/li>\n        <\/ul>\n    <div class=\"tabs\">\n            <div class=\"tab\" id=\"c78ece9e2b0\" style=\"display: block\">\n<p><img loading=\"lazy\" alt=\"Low voltage alarm circuit built on a breadboard\" src=\"\/user\/pages\/02.blog\/zener-diode-low-voltage-alarm\/battery-alarm-circuit_Breadboard.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<\/div>\n            <div class=\"tab\" id=\"c78ece9e2b1\" style=\"display: none\">\n<p><img loading=\"lazy\" alt=\"Schematic for the low voltage alarm circuit\" src=\"\/user\/pages\/02.blog\/zener-diode-low-voltage-alarm\/battery-alarm-circuit.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<\/div>\n        <\/div>\n<\/div>\n\n<h2 id=\"the-result\">The Result<a href=\"#the-result\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>To use the circuit, connect it to the battery in parallel to the load. As soon as the battery voltage drops below 12...<\/p>","tags":["electronics","diodes"],"image":"\/user\/pages\/02.blog\/zener-diode-low-voltage-alarm\/zener-diode-low-voltage-alarm.jpg?g-982d5237"},{"title":"Zener Diodes as Voltage Reference","date_published":"2023-02-13T08:00:00+01:00","id":"https:\/\/devxplained.eu\/en\/blog\/zener-diodes-as-voltage-reference","url":"https:\/\/devxplained.eu\/en\/blog\/zener-diodes-as-voltage-reference","content_html":"<p><strong>What can we use zener diodes for? This time, we look at their use as voltage references.<\/strong><\/p>\n\n<h2 id=\"zener-diodes-as-voltage-r\">Zener Diodes as Voltage Reference<a href=\"#zener-diodes-as-voltage-r\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>The special property of zener diodes is that they have a specified reverse breakdown voltage. This property especially useful for circuits that require fixed voltage reference. In circuits with varying supply voltage, e.g., battery operated ones, a simple voltage divider is not enough for this. Using a zener diode is one way to solve this issue. In this article we are going to look at how this works and discuss, when to and when not to use a zener for this purpose.<\/p>\n<p>How can we build voltage reference using a zener? Well, we simply select a zener for your desired voltage and use it together with a current limiting resistor.<\/p>\n<p><img loading=\"lazy\" alt=\"Use of a zener diode as voltage reference\" src=\"\/user\/pages\/02.blog\/zener-diodes-as-voltage-reference\/zener-as-voltage-reference.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>If the voltage is above the zener voltage, the diode conducts. It clamps the output voltage to the zener voltage while the remaining voltage is dropped across the zener diode itself. Of course, the zener diode can only provide a bypass for a limited amount of current. To prevent it from getting damaged, we need the resistor to limit the maximum current.<\/p>\n<p>That's simple enough, but where would you use such a circuit?<\/p>\n<h2 id=\"how-to-use-a-voltage-refe\">How to Use a Voltage Reference?<a href=\"#how-to-use-a-voltage-refe\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>A circuit that outputs a specific voltage? It is easy to think of a voltage source here, but that is not what a voltage reference is. Voltage references should be used together with high impedance inputs like the ones of microcontrollers, op amps or comparators. What does that mean? In practice, it means, that they have an input that draws a very small current. While voltage references can provide a fixed voltage, they can provide almost no current.<\/p>\n<p>Let's have a look at an example circuit that uses a zener diode as a voltage reference in its intended way:<\/p>\n<div class=\"tabs-wrapper ui-theme-default top-left\">\n    <ul class=\"tabs-nav\">\n                    <li class=\"current\"><a href=\"#8a079df3a30\" id=\"Tab0\" rel=\"tab\">Breadboard<\/a><\/li>\n                    <li><a href=\"#8a079df3a31\" id=\"Tab1\" rel=\"tab\">Schematic<\/a><\/li>\n        <\/ul>\n    <div class=\"tabs\">\n            <div class=\"tab\" id=\"8a079df3a30\" style=\"display: block\">\n<p><img loading=\"lazy\" alt=\"Zener as voltage reference for a comparator circuit\" src=\"\/user\/pages\/02.blog\/zener-diodes-as-voltage-reference\/zener-as-reference-circuit_Breadboard.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<\/div>\n            <div class=\"tab\" id=\"8a079df3a31\" style=\"display: none\">\n<p><img loading=\"lazy\" alt=\"Schematic for the comparator circuit with a zener as voltage reference\" src=\"\/user\/pages\/02.blog\/zener-diodes-as-voltage-reference\/zener-as-reference-circuit.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<\/div>\n        <\/div>\n<\/div>\n\n<p>The circuit uses a 9 V zener diode as voltage reference for an LM393 comparator.\nA comparator compares the voltage as its two inputs: if the voltage at the non-inverting input (+) is higher than the one on its inverting input (-), its output is high otherwise it is low.<\/p>\n<p>In this example, a potentiometer is connected to the non-inverting input and the 9 V reference voltage connects to the inverting input. The comparator's output becomes high, when the output voltage of the potentiometer is above 9 V, otherwise it is low. The circuit has an LED connected to the comparator's output. This LED turns on, if the potentiometers output is below 9V. <\/p>\n<div class=\"notices blue\">\n<p><strong>Didn't expect that?<\/strong><br>\nThe circuit uses the LED in an active-low configuration. Its positive side connects to the supply voltage and the LM393 switches its connection to ground. This might be an odd choice at first, however, the reason for this, is the way the LM393 works. The LM393 has an open-collector output, which means that it only supports the two output states floating (not connected) and low (connected to ground).<\/p>\n<\/div>\n<h2 id=\"conclusion\">Conclusion<a href=\"#conclusion\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p><strong>What can you<\/strong>...<\/p>","tags":["electronics","diodes"],"image":"\/user\/pages\/02.blog\/zener-diodes-as-voltage-reference\/zener-diodes-as-voltage-reference.jpg?g-982d5237"},{"title":"Avalanche Breakdown","date_published":"2023-01-09T08:00:00+01:00","id":"https:\/\/devxplained.eu\/en\/blog\/avalanche-breakdown","url":"https:\/\/devxplained.eu\/en\/blog\/avalanche-breakdown","content_html":"<p><strong>Let's learn more about the second important breakdown effect in zener diodes: the avalanche breakdown.<\/strong><\/p>\n\n<h2 id=\"avalanche-breakdown\">Avalanche Breakdown<a href=\"#avalanche-breakdown\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>There are two noteworthy breakdown effects in zener diodes: the zener effect and the avalanche breakdown. This time, we are going to take a deeper look at the latter.<\/p>\n<p>The avalanche breakdown is especially important to zener diodes with breakdown voltages above 5 V. It is identifiable by the strong increase of conductivity, once the breakdown voltage is exceeded. This can be easily seen in the I-V curve. Something drastic seems to happen here. Let's take a look at the underlying physical process, that does not only apply to zener diodes, but is of a more general significance. Ready to learn more?<\/p>\n<p><img loading=\"lazy\" alt=\"The avalanche breakdown shows itself in the steep I-V curve for zener diodes with a breakdown voltage above 5 V\" src=\"\/user\/pages\/02.blog\/avalanche-breakdown\/iv-zener-and-avalanche-diodes.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<div class=\"notices yellow\">\n<p><strong>Disclaimer:<\/strong> I'm not a physicist and semiconductors are an extremely complicated topic. I cannot guarantee for correctness of my explanations. For the ease of understanding some details might be left out or presented in an over simplified manner. If you think, that parts of this article need correction, contact me at <i class=\"fa fa-envelope-o\"><\/i> <a href=\"mailto:feedback@devxplained.eu\">feedback@devxplained.eu<\/a>.<\/p>\n<\/div>\n<h2 id=\"how-does-it-work\">How does it work?<a href=\"#how-does-it-work\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Luckily, the avalanche breakdown and the underlying physical process are much easier to understand than the zener effect. Similar to the zener effect, the avalanche breakdown is caused by high electric field strengths. The underlying physical effect is, however, a different one: impact ionization.\nLet's see what it is.<\/p>\n<h3 id=\"impact-ionization\">Impact Ionization<a href=\"#impact-ionization\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h3>\n<p>Even without externally applied fields electrons can move in the semiconductor material, which is e.g., caused by thermal energy. They randomly collide with other electrons and in this process give up part of their kinetic energy to them. It's an ever ongoing process of electrons colliding which each other, a constant back and forth of excitation and relaxation.<\/p>\n<p>High electric field strengths always imply high acceleration forces to electrically charged particles like electrons.\nThings get interesting once the kinetic energy of electrons exceeds a certain level. At this point, once they hit another electron, they do not simply loose part of their energy to it, but set free new charge carriers. <\/p>\n<p>This process is called impact ionization, where ionization in general is just another term for the creation of new charge carriers from an atom.\nThe image below visualizes the ionization process. Due to the colliding electron the atom loses one of its electrons and itself becomes a positively charged ion. Since we talk about semiconductors, we are better off saying: the colliding electron causes there to be an additional free electron and a new electron hole in the semiconductor material. <\/p>\n<p><img loading=\"lazy\" alt=\"Impact ionization visualized in the Bohr model\" src=\"\/user\/pages\/02.blog\/avalanche-breakdown\/avalanche-breakdown-bohr-model.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<h3 id=\"from-impact-ionization-to\">From Impact Ionization to an Electron Avalanche<a href=\"#from-impact-ionization-to\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h3>\n<p>What happens with this newly generated charge carries? Well, they get themselves accelerated by the electric field and start colliding with electrons in other atoms, where they can again cause impact ionization. This causes a chain-reaction, the so-called electron avalanche. The number of free charge carriers rises exponentially, and the material becomes more and more conductive.<\/p>\n<p><img loading=\"lazy\" alt=\"A chain-reaction is caused: the electron avalanche\" src=\"\/user\/pages\/02.blog\/avalanche-breakdown\/electron-avalanche.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<h3 id=\"avalanche-breakdown-in-di\">Avalanche Breakdown in Diodes<a href=\"#avalanche-breakdown-in-di\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h3>\n<p>If we look at how diodes work, we can easily see how such an electron...<\/p>","tags":["electronics","physics","diodes"],"image":"\/user\/pages\/02.blog\/avalanche-breakdown\/avalanche-breakdown.jpg?g-982d5237"},{"title":"Building Dark Activated LED Lights","date_published":"2022-12-12T08:00:00+01:00","id":"https:\/\/devxplained.eu\/en\/blog\/building-dark-activated-led-lights","url":"https:\/\/devxplained.eu\/en\/blog\/building-dark-activated-led-lights","content_html":"<p><strong>Let's learn how to build dark activated LED lights to brighten up the dark time of the year.<\/strong><\/p>\n\n<h2 id=\"building-dark-activated-l\">Building Dark Activated LED Lights<a href=\"#building-dark-activated-l\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>It's winter, it's cold, and it's dark outside. What's better than bringing some light into this darkness. In this year's DIY project, we are going to build our own dark activated LED lights from a cheap battery operated LED string.<\/p>\n<p>Here is what we need:<\/p>\n<ul>\n<li>a battery-powered LED string<\/li>\n<li>an LDR<\/li>\n<li>a resistor between 1 k&Omega; - 1 M&Omega; (100 k&Omega; recommended)<\/li>\n<li>a MOSFET (FQP30N06L)<\/li>\n<li>a piece of perfboard (14x5 holes)<\/li>\n<\/ul>\n<p><img loading=\"lazy\" alt=\"Required material\" src=\"\/images\/r\/e\/q\/u\/i\/required-material-09fb71d5.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/required-material@2x.jpg?g-982d5237 4096w, \/images\/r\/e\/q\/u\/i\/required-material-09fb71d5.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<p>Additionally, you are going to need to following tools:<\/p>\n<ul>\n<li>a soldering iron and solder<\/li>\n<li>a wire cutter<\/li>\n<li>a 3.3 mm drill<\/li>\n<li>a pencil<\/li>\n<\/ul>\n<h2 id=\"the-circuit\">The Circuit<a href=\"#the-circuit\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Let's have a look at the circuit for this project. The LEDs shall light up when it gets dark outside. We can achieve this by using a simple transistor circuit which is shown below.<\/p>\n<p><img loading=\"lazy\" alt=\"Circuit diagram for the dark activated LED lights\" src=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/schematic.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>The LDR and the resistor R1 form a voltage divider. The resistance of the LDR increases the darker it gets. A high resistance of the LDR means a higher voltage at the MOSFETs gate. As soon as the gate voltage crosses the 1 V mark the MOSFET starts to turn on. <\/p>\n<p>To control at which brightness level that happens we can tune the value for resistor R1. The optimal value depends on how you want to use your LED string. If it you want it to only turn on, if it is fully dark you require a high value like 470 k&Omega; or more. If you want it to also light up on darker days, you need a lower value like 10 k&Omega;. <\/p>\n<p>I can only encourage you to experiment, until you find the value that fits your use case. If you don't feel like experimenting, I can recommend you to use 100 k&Omega;. It should fit for most indoor use cases.<\/p>\n<h2 id=\"let-s-build-it\">Let's build it!<a href=\"#let-s-build-it\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<div class=\"owl-carousel owl-theme\" id=\"owl-9da2877542\">\n    \n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 1:<\/strong> Let's go! As a first step, we place the components on the perfboard without soldering them in yet. If you want to, you can already cut them to the right length.<\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 1: Placing the components to cut them to the right length\" src=\"\/images\/s\/t\/e\/p\/-\/step-1-655947d8.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-1@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-1-655947d8.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 2:<\/strong> With the components in place, we can use a pencil to mark the positions in which we want to drill the holes for the wires.<\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 2: Marking the spots for the holes\" src=\"\/images\/s\/t\/e\/p\/-\/step-2-617028c8.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-2@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-2-617028c8.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 3:<\/strong> For drilling, we need to remove the components again and make sure to safely clamp the perfboard on a piece of scrap wood. We can then drill the two holes.<\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 3: Drilling the holes\" src=\"\/images\/s\/t\/e\/p\/-\/step-3-7e0bc258.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-3@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-3-7e0bc258.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 4:<\/strong> With the holes made, we can now place the components to finally solder them in. <\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 4: Placing the components to solder them in\" src=\"\/images\/s\/t\/e\/p\/-\/step-4-748c2209.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-4@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-4-748c2209.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 5:<\/strong> After that, we connect the resistor and the LDR to the MOSFETs gate with a solder bridge.<\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 5: Soldering the LDR and the resistor to the MOSFETs gate\" src=\"\/images\/s\/t\/e\/p\/-\/step-5-74a3bf74.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-5@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-5-74a3bf74.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 6:<\/strong> Next, we need to attach our LED string and its battery holder. For this, cut its wire in half and tin the ends of each side.<\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 6: Cutting and tinning the wires of the LED string\" src=\"\/images\/s\/t\/e\/p\/-\/step-6-4e811a52.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-6@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-6-4e811a52.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 7:<\/strong> Pull the wire through the holes and fixate them in place with a knot. The knot serves as a strain relieve.<\/p>\n<\/div>\n<div class=\"slider-item-image\">\n<p><img loading=\"lazy\" alt=\"Step 7: Pull the wire through the holes, fix them in place with a knot as strain relieve\" src=\"\/images\/s\/t\/e\/p\/-\/step-7-68ee165c.jpg?g-982d5237\" srcset=\"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/step-7@2x.jpg?g-982d5237 4096w, \/images\/s\/t\/e\/p\/-\/step-7-68ee165c.jpg?g-982d5237 2048w\" sizes=\"100vw\"><\/p>\n<\/div>\n<\/div>\n<div class=\"slider-item\">\n<div class=\"slider-item-text\">\n<p><strong>Step 8:<\/strong> Now...<\/p><\/div><\/div><\/div>","tags":["light","christmas","DIY","transistors"],"image":"\/user\/pages\/02.blog\/building-dark-activated-led-lights\/building-dark-activated-led-lights.jpg?g-982d5237"},{"title":"Zener Effect","date_published":"2022-11-14T08:00:00+01:00","id":"https:\/\/devxplained.eu\/en\/blog\/zener-effect","url":"https:\/\/devxplained.eu\/en\/blog\/zener-effect","content_html":"<p><strong>The zener effect is the dominant breakdown effect in low voltage zener diodes. Let's take some time to learn more about it.<\/strong><\/p>\n\n<h2 id=\"zener-effect\">Zener Effect<a href=\"#zener-effect\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Zener diodes are diodes with a known breakdown voltage, which is called the zener voltage. There are two effects, that cause this breakdown: the zener effect and the avalanche breakdown. The zener effect is the dominant breakdown effect at voltages below 5 V. Compared with the avalanche breakdown, it is noticeable by it less steep I-V curve. Today, we want to take a closer look at it.<\/p>\n<p><img loading=\"lazy\" alt=\"IV curve for zener diodes with different zener voltages\" src=\"\/user\/pages\/02.blog\/zener-effect\/iv-zener-and-avalanche-diodes.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>The zener effect is named after Clarence M. Zener, who was an American physicist researching on breakdown effects in different materials. In 1934, he published a theory predicting the properties of the zener breakdown. The first zener diode was built in 1950 by Bell Labs and named after him. But what was it that Zener predicted? And how does the zener effect work in semiconductors? Are you ready for a little deep dive into semiconductor physics?<\/p>\n<div class=\"notices yellow\">\n<p><strong>Disclaimer:<\/strong> I'm not a physicist and semiconductors are an extremely complicated topic. I cannot guarantee for correctness of my explanations. For the ease of understanding some details might be left out or presented in an over simplified manner. If you think, that parts of this article need correction, contact me at <i class=\"fa fa-envelope-o\"><\/i> <a href=\"mailto:feedback@devxplained.eu\">feedback@devxplained.eu<\/a>.<\/p>\n<\/div>\n<h2 id=\"how-does-it-work\">How does it work?<a href=\"#how-does-it-work\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>To understand how the zener effect in zener diodes work, we first need to recap, what happens on a p-n junction. I already described this in lengths in a dedicated <a href=\"https:\/\/devxplained.eu\/en\/blog\/p-n-junction\">article on the p-n junction<\/a>, however, to understand the zener effect, we should take another look at the p-n junction &ndash; this time with the help of the band model.<\/p>\n<p>If you followed up on my past articles, the following image might be familiar to you. It shows the process of electron excitation and relaxation in semiconductors in the band model. I'll use this image to recap the most essential parts about the band model for you.\n<img loading=\"lazy\" alt=\"Excitation and relaxation in the band model\" src=\"\/user\/pages\/02.blog\/zener-effect\/bandmodel-excitation-and-relaxation.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>The band model is based on the quantum mechanic observations, that electrons are not located at fixed positions in an atom. Instead, their positions have to be described probabilistically. However, this does not mean that the electrons are scattered totally random around the nucleus. Around the nucleus there are different energy bands in which the electrons are likely located. In between these bands there are gaps: the so-called forbidden zones or band gaps. These gaps described a region in which electrons are very unlikely to be found. An electron cannot simply move into another band. It needs enough energy to jump across the band gap into the next energy band. This happens at random when electrons collide with another, e.g., due to internal thermal motion, and as well under the external influences like colliding photons.<\/p>\n<p>The most interesting energy bands in the context of electronics are the valence band and the conduction band. The conduction band is the first band in which electrons can freely move between atoms,...<\/p>","tags":["electronics","physics","diodes"],"image":"\/user\/pages\/02.blog\/zener-effect\/zener-effect.jpg?g-982d5237"},{"title":"Zener Diodes","date_published":"2022-10-17T08:00:00+02:00","id":"https:\/\/devxplained.eu\/en\/blog\/zener-diodes","url":"https:\/\/devxplained.eu\/en\/blog\/zener-diodes","content_html":"<p><strong>It is a special type of diode designed to operate reverse biased: the zener diode.<\/strong><\/p>\n\n<h2 id=\"zener-diodes\">Zener Diodes<a href=\"#zener-diodes\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>Today, we are going to take a look at the so-called zener diodes. They are a special kind of diodes that are build with an exactly known breakdown voltage.\nIn circuit diagrams they are denoted as shown below. The first symbol is the standard IEC symbol, however, you can often also find the two symbols from the bottom row to be used in schematics. Beware, that especially the last one can be easily confused with the Schottky diode symbol. Luckily, in most cases the breakdown voltage is denoted right next to the symbol so that the component can be clearly identified as a zener diode.<\/p>\n<p><img loading=\"lazy\" alt=\"Circuit symbol for zener diodes\" src=\"\/user\/pages\/02.blog\/zener-diodes\/diodes.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>Zener diodes act just like normal diodes when forward biased, however, that is not the way zener diodes are meant to be used. The typical zener diode circuits use it in reverse biased configuration, in which it starts to conduct, as soon as its known breakdown voltage is exceeded. This property can be used for a variety of different circuits like, e.g, overvoltage protection, voltage stabilization or voltage references.<\/p>\n<h2 id=\"properties-of-zener-diode\">Properties of Zener Diodes<a href=\"#properties-of-zener-diode\" class=\"toc-anchor after\" data-anchor-icon=\"#\" aria-label=\"Anchor\"><\/a><\/h2>\n<p>What are the properties of zener diodes? Zener diodes are using highly doped silicon. Due to the high doping level the depletion region on the junction becomes very narrow.\nThe narrow junction is what defines the main properties of zener diodes:<\/p>\n<ul>\n<li>Zener diodes have a low breakdown voltage, which makes them ill-suited for the use as rectifier diodes<\/li>\n<li>Due to the narrow depletion region, zener diodes have a high junction capacitance, which makes them ill-suited for the use as signal diodes<\/li>\n<\/ul>\n<p>So you can see, that zener diodes have primarily disadvantages when used like normal diodes. It is their exactly known breakdown voltage that makes them special. The breakdown voltage is dependent on the exact doping levels. This makes it possible to design zener diodes for different breakdown voltages.\nThe most important characteristics of a zener diode are:<\/p>\n<ul>\n<li>the zener voltage <span class=\"mathjax mathjax--inline\">\\(V_{Z}\\)<\/span> which is equivalent to the breakdown voltage <span class=\"mathjax mathjax--inline\">\\(V_{BR}\\)<\/span><\/li>\n<li>the maximum power dissipation <span class=\"mathjax mathjax--inline\">\\(P_{tot}\\)<\/span><\/li>\n<\/ul>\n<p>The power dissipation can be calculated just like for normal diodes, but because zener diodes are used reversed biased, you need to multiply the current <span class=\"mathjax mathjax--inline\">\\(I\\)<\/span> with the zener voltage <span class=\"mathjax mathjax--inline\">\\(V_{Z}\\)<\/span> instead of the forward voltage <span class=\"mathjax mathjax--inline\">\\(V_F\\)<\/span>:<br>\n<span class=\"mathjax mathjax--inline\">\\(P_{tot} = V_Z \\cdot I\\)<\/span><\/p>\n<p>The graph below shows the I-V curve for zener diodes with different breakdown voltages. When forward-biased they are good conductors above 0.7 V, just like normal diodes. Reverse biased, each diode starts to conduct at its designated zener voltage.<\/p>\n<p><img loading=\"lazy\" alt=\"I-V curve for zener diodes with different breakdown voltages\" src=\"\/user\/pages\/02.blog\/zener-diodes\/iv-zener-and-avalanche-diodes.svg?decoding=auto&amp;fetchpriority=auto&amp;g-982d5237\"><\/p>\n<p>You may notice, that the I-V curve for diodes with a low breakdown voltage differs from the one with higher breakdown voltages. For the higher voltage ones the curve is much more steep than for the lower voltage ones.\nThis is because there are two different physical effects causing the breakdown: the zener effect and the avalanche breakdown. At voltages below 5 V the zener effect is dominant....<\/p>","tags":["electronics","diodes"],"image":"\/user\/pages\/02.blog\/zener-diodes\/zener-diodes.jpg?g-982d5237"}]}
