In electrical stores, capacitors can most often be seen in the form of a cylinder, inside of which there are many strips of plates and dielectrics.
The capacitor is part electrical circuit, consisting of 2 electrodes that are capable of accumulating, focusing or transmitting current to other devices. Structurally, the electrodes are capacitor plates with opposite charges. In order for the device to work, a dielectric is placed between the plates - an element that prevents the two plates from touching each other.
The definition of condenser comes from the Latin word “condenso”, which means compaction, concentration.
Elements for soldering containers are used to transport, measure, redirect and transmit electricity and signals.
Every novice radio amateur often asks the question: what is a capacitor for? Beginners do not understand why it is needed and mistakenly believe that it can fully replace a battery or power supply.
All radio devices include capacitors, transistors and resistors. These elements make up a board or an entire module in circuits with static values, which makes it the basis for any electrical appliance, from a small iron to industrial devices.
The most common uses of capacitors are:
The purpose of the capacitor and its functions are determined by the purposes of use:
The design of the capacitor is determined by the type of dielectric. It comes in the following types:
The elements of the radio board differ in the type of capacitance change:
Let's look at how a capacitor works when connected to a power source:
The capacitance of a capacitor is determined by calculating the ratio of the charge of one conductor to its potential power.
Important! The dielectric is also capable of removing the resulting voltage on the capacitor during operation of the device.
The characteristics are conventionally divided into points:
The capacitance of the capacitor depends on the type of dielectric and is indicated on the case, measured in uF or uF. It ranges from 0 to 9,999 pF in picofarads, while in microfarads it ranges from 10,000 pF to 9,999 µF. These characteristics are specified in state standard GOST 2.702.
Note! The larger the electrolyte capacity, the longer the charging time, and the more charge the device can transfer.
The greater the load or power of the device, the shorter the discharge time. In this case, resistance plays an important role, since the amount of outgoing electrical flow depends on it.
The main part of the capacitor is the dielectric. It has the following number of characteristics that affect the power of the equipment:
Good to know! The abbreviation “AC” located on the element body means AC voltage. The accumulated voltage on the capacitor cannot be used or transmitted - it must be extinguished.
The capacitor acts as:
If you regularly create electrical diagrams, you probably used capacitors. It's a standard circuit component, just like resistor, that you just grab off the shelf without a second thought. We use capacitors to smooth out voltage/current ripple, to match loads, as a power source for low-power devices, and other applications.
But a capacitor is not just a bubble with two wires and a couple of parameters - operating voltage and capacitance. There is a huge array of technologies and materials with different properties, used to create capacitors. And although in most cases almost any capacitor of suitable capacity will do for any task, good understanding how these devices work can help you choose not just the right one, but the best fit. If you have ever had a problem with temperature stability or the task of finding the source of additional noise, you will appreciate the information in this article.
Capacitance is measured in farads: a capacitor of one farad produces a voltage of one volt if it contains a charge of one coulomb. Like many other SI units, it's an impractical size, so unless you count supercapacitors, which we won't talk about here, you'll likely end up with micro-, nano-, and picofarads. The capacitance of any capacitor can be derived from its dimensions and dielectric properties - if interested, the formula for this can be found on Wikipedia. There is no need to memorize it unless you are studying for an exam - but it does contain one useful fact. The capacitance is proportional to the dielectric constant εr of the dielectric used, which has resulted in a variety of capacitors being commercially available using different dielectric materials to achieve larger capacitances or improve voltage characteristics.
Aluminum electrolytic capacitors use an anodic oxidation layer on an aluminum sheet as one dielectric plate, and the electrolyte from an electrochemical cell as the other plate. The presence of an electrochemical cell makes them polar, that is, the DC voltage must be applied in one direction, and the anodized plate must be the anode, or positive.
In practice, their plates are made in the form of a sandwich of aluminum foil, wrapped in a cylinder and located in aluminum can. The operating voltage depends on the depth of the anodized layer.
Electrolytic capacitors have the largest capacitance among common ones, from 0.1 to thousands of microfarads. Due to the close packing of the electrochemical cell, they have a large equivalent series inductance (ESI, or effective inductance), which is why they cannot be used on high frequencies. They are typically used for power smoothing and decoupling as well as coupling at audio frequencies.
Tantalum electrolytic capacitors are manufactured as a sintered tantalum anode with a large surface area on which a thick layer of oxide is grown and then a manganese dioxide electrolyte is placed as the cathode. The combination of the large surface area and dielectric properties of tantalum oxide results in high capacitance per volume. As a result, such capacitors are much smaller than aluminum capacitors of comparable capacity. Like the latter, tantalum capacitors have polarity, so direct current must flow in exactly one direction.
Their available capacitance varies from 0.1 to several hundred microfarads. They have much lower leakage resistance and equivalent series resistance (ESR), which is why they are used in testing, measuring instruments and high-quality audio devices – where these properties are useful.
In the case of tantalum capacitors, it is necessary to especially monitor the failure status; it happens that they catch fire. Amorphous tantalum oxide is a good dielectric, and in crystalline form it becomes a good conductor. Improper use of a tantalum capacitor - for example, applying too much inrush current - can cause the dielectric to change form, which will increase the current passing through it. It is true that earlier generations of tantalum capacitors had a reputation for fire problems, and improved manufacturing methods have led to more reliable products.
Polypropylene capacitors are used in circuits that require good thermal and frequency stability. They are also used in power systems, to suppress EMI, in systems using high voltage alternating currents.
Polyester capacitors, although they do not have the same temperature and frequency characteristics, are cheap and can withstand high temperatures when soldering for surface mounting. Because of this, they are used in circuits intended for use in non-critical applications.
Polyethylene naphthalate capacitors. They do not have stable temperature and frequency characteristics, but can withstand much higher temperatures and stresses compared to polyester ones.
Polyethylene sulfide capacitors have the temperature and frequency characteristics of polypropylene, and in addition can withstand high temperatures.
In old equipment you can come across polycarbonate and polystyrene capacitors, but now they are no longer used.
The history of ceramic capacitors is quite long - they have been used from the first decades of the last century to the present day. Early capacitors were a single layer of ceramic, metallized on both sides. Later ones are also multilayer, where plates with metallization and ceramics are interspersed. Depending on the dielectric, their capacitances vary from 1 pF to tens of microfarads, and voltages reach kilovolts. In all electronics industries where low capacitance is required, both single-layer ceramic disks and multi-layer surface-mount stack capacitors can be found.
The easiest way to classify ceramic capacitors is by dielectrics, since they are what give the capacitor all its properties. Dielectrics are classified according to three-letter codes, which encrypt their operating temperature and stability.
C0G has better stability in capacitance with respect to temperature, frequency and voltage. Used in high-frequency circuits and other high-speed circuits.
X7R do not have such good characteristics by temperature and voltage, therefore they are used in less critical cases. This usually includes decoupling and various universal applications.
Y5V have much higher capacity, but their temperature and voltage characteristics are even lower. Also used for decoupling and in various general purpose applications.
Since ceramics often also have piezoelectric properties, some ceramic capacitors also exhibit a microphonic effect. If you have worked with high voltages and frequencies in the audio range, for example, in the case of tube amplifiers or electrostatics, you could hear the capacitors “singing”. If you used a piezoelectric capacitor to provide frequency stabilization, you might find that its sound is modulated by the vibration of its surroundings.
As we already mentioned, this article does not aim to cover all capacitor technologies. Taking a look at the electronics catalog you will find that some of the technologies available are not covered here. Some offers from catalogs are already outdated, or have such a narrow niche that you most often will not come across them. We only hoped to dispel some of the mystery about popular models capacitors, and help you select the right components when designing your own devices. If we've whetted your appetite, you may want to check out our article on inductors.
Please write about any inaccuracies or errors you find via
Constant voltage and set the voltage on his crocodiles to 12 Volts. We also take a 12 Volt light bulb. Now we insert a capacitor between one probe of the power supply and the light bulb:
Nope, it doesn't burn.
But if you do it directly, it lights up:
This begs the conclusion: DC current does not flow through the capacitor!
To be honest, at the very initial moment of applying voltage, the current still flows for a fraction of a second. It all depends on the capacitance of the capacitor.
So, to find out whether AC current is flowing through the capacitor, we need an alternator. I think this frequency generator will do just fine:
Because Chinese generator I have a very weak one, then instead of a light bulb load we will use a simple 100 Ohm. Let’s also take a capacitor with a capacity of 1 microfarad:
We solder something like this and send a signal from the frequency generator:
Then he gets down to business. What is an oscilloscope and what it is used for, read here. We will use two channels at once. Two signals will be displayed on one screen at once. Here on the screen you can already see interference from the 220 Volt network. Do not pay attention.
We will apply alternating voltage and watch the signals, as professional electronics engineers say, at the input and output. Simultaneously.
It will all look something like this:
So, if our frequency is zero, then this means constant current. As we have already seen, the capacitor does not allow direct current to pass through. This seems to have been sorted out. But what happens if you apply a sinusoid with a frequency of 100 Hertz?
On the oscilloscope display I displayed parameters such as signal frequency and amplitude: F is the frequency Ma – amplitude (these parameters are marked with a white arrow). The first channel is marked in red, and the second channel in yellow, for ease of perception.
The red sine wave shows the signal that the Chinese frequency generator gives us. The yellow sine wave is what we already get at the load. In our case, the load is a resistor. Well, that's all.
As you can see in the oscillogram above, I supply a sinusoidal signal from the generator with a frequency of 100 Hertz and an amplitude of 2 Volts. On the resistor we already see a signal with the same frequency (yellow signal), but its amplitude is some 136 millivolts. Moreover, the signal turned out to be somewhat “shaggy”. This is due to the so-called ““. Noise is a signal with small amplitude and random voltage changes. It can be caused by the radio elements themselves, or it can also be interference that is caught from the surrounding space. For example, a resistor “makes noise” very well. This means that the “shaggyness” of the signal is the sum of a sinusoid and noise.
The amplitude of the yellow signal has become smaller, and even the graph of the yellow signal shifts to the left, that is, it is ahead of the red signal, or in scientific language, it appears phase shift. It is the phase that is ahead, not the signal itself. If the signal itself was ahead, then we would have the signal on the resistor appear in time earlier than the signal applied to it through the capacitor. The result would be some kind of time travel :-), which, of course, is impossible.
Phase shift- This difference between the initial phases of two measured quantities. In this case, tension. In order to measure the phase shift, there must be a condition that these signals same frequency. The amplitude can be any. The figure below shows this very phase shift or, as it is also called, phase difference:
Let's increase the frequency on the generator to 500 Hertz
The resistor has already received 560 millivolts. The phase shift decreases.
We increase the frequency to 1 KiloHertz
At the output we already have 1 Volt.
Set the frequency to 5 Kilohertz
The amplitude is 1.84 Volts and the phase shift is clearly smaller
Increase to 10 Kilohertz
The amplitude is almost the same as at the input. The phase shift is less noticeable.
We set 100 Kilohertz:
There is almost no phase shift. The amplitude is almost the same as at the input, that is, 2 Volts.
From here we draw profound conclusions:
The higher the frequency, the less resistance the capacitor has to alternating current. The phase shift decreases with increasing frequency to almost zero. On indefinitely low frequencies its value is 90 degrees orπ/2 .
If you plot a slice of the graph, you will get something like this:
I plotted voltage vertically and frequency horizontally.
So, we have learned that the resistance of a capacitor depends on frequency. But does it only depend on frequency? Let's take a capacitor with a capacity of 0.1 microfarad, that is, a nominal value 10 times less than the previous one, and run it again at the same frequencies.
Let's look and analyze the values:
Carefully compare the amplitude values of the yellow signal at the same frequency, but with different capacitor values. For example, at a frequency of 100 Hertz and a capacitor value of 1 μF, the amplitude of the yellow signal was 136 millivolts, and at the same frequency, the amplitude of the yellow signal, but with a capacitor of 0.1 μF, was already 101 millivolts (in reality, even less due to interference ). At a frequency of 500 Hertz - 560 millivolts and 106 millivolts, respectively, at a frequency of 1 Kilohertz - 1 Volt and 136 millivolts, and so on.
From here the conclusion suggests itself: As the value of a capacitor decreases, its resistance increases.
Using physical and mathematical transformations, physicists and mathematicians have derived a formula for calculating the resistance of a capacitor. Please love and respect:
Where, X C is the resistance of the capacitor, Ohm
P - constant and equals approximately 3.14
F– frequency, measured in Hertz
WITH– capacitance, measured in Farads
So, put the frequency in this formula at zero Hertz. A frequency of zero Hertz is direct current. What will happen? 1/0=infinity or very high resistance. In short, a broken circuit.
Looking ahead, I can say that in this experiment we obtained (high-pass filter). Using a simple capacitor and resistor, and applying such a filter to the speaker somewhere in the audio equipment, we will only hear squeaky high tones in the speaker. But the bass frequency will be dampened by such a filter. The dependence of capacitor resistance on frequency is very widely used in radio electronics, especially in various filters where it is necessary to suppress one frequency and pass another.
Rice. 19. Minimum permissible distance between the housing of an aluminum electrolytic capacitor and the wall of the equipment housing
Do not obstruct the operation of ventilation systems unless otherwise specified in catalogs or technical specifications equipment. Too small a gap between the capacitor body and the device body can negatively affect the operation of the ventilation system and lead to an explosion of the capacitor.
Attention!
- The information contained in this article is subject to change to improve product quality without prior notice. Therefore, please check the latest specifications before ordering electrolytic capacitors.
- The general characteristics, reliability data and other parameters of aluminum electrolytic capacitors given in this article should not be considered as guaranteed values - they are standard, typical values only.
- For correct use electrolytic capacitors, please first carefully read the application recommendations given in this article.
They are used in timers because resistors allow for slow charging and discharging. Inductors along with capacitors are present in the circuits of oscillatory circuits of receiving and transmitting devices. IN various designs power supplies, they effectively smooth out voltage ripples after the rectification process.
It passes through capacitors easily, but is delayed. This makes it possible to produce filters for various purposes. In electrical and radio electronic circuits, capacitors help slow down processes such as voltage increases or decreases.
The basic principle of operation of a capacitor is its ability to store electric charge. That is, it can be charged or discharged at the right time. This property is most clearly manifested when a capacitor is connected in parallel or in series with an inductor in transmitter or radio receiver circuits.
This connection allows you to obtain a periodic change in polarity on the plates. First, the first plate is charged with a positive charge, and then the second plate takes on a negative charge. After complete discharge, charging occurs in reverse direction. Instead of a positive charge, the plate receives a negative charge and, conversely, the negative plate becomes positively charged. This polarity change occurs after each charge and discharge. This operating principle is the basis for generators installed in analog transceiver devices.
When considering the principle of operation of a capacitor, one should not forget about such a characteristic as electrical capacitance. First of all, it lies in the ability of a capacitor to retain an electrical charge. That is, the higher the capacity, the higher value charge can be saved.
The electrical capacitance of a capacitor is measured in farads and is designated by the letter F. However, one farad is a very large capacitance, so in practice smaller units such as micro-, nano- and picofarads are used.
It presents a certain complexity due to different labeling options.
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