A favorite project on the forum is the construction of a power supply. If you're going to be building electronic projects, it soon becomes tiresome to always be buying and using up batteries, so the desirability of a grid powered supply quickly becomes apparent!
The kind of power supply project to be built is going to be transformer based for safety reasons. It may be regulated or unregulated, but the basic circuit is a small, relatively low voltage transformer, followed by a rectifier and an electrolytic capacitor for filtering.
I'm going to be dealing with only one very specific topic, but the beginner should read this description of power supply design before continuing here:
http://www.zen22142.zen.co.uk/Design/dcpsu.htm
Beginning power supply builders soon discover that a given transformer can't supply as many DC amps when used in a power supply as the transformer is rated for by the manufacturer. This is because the transformer rating is for an AC resistive load which draws a current whose waveshape is a sine wave, like the waveform of the grid voltage. When the transformer is used in a power supply with a capacitor filter, the current drawn from the secondary is no longer a sine wave; it's a narrow, peaked waveform, and such a waveform causes extra heating in the transformer. This is why the transformer must be derated when used in a rectifier/capacitor power supply, and that's what this post is all about.
I've attached an image showing a scope capture of the voltage and currents in a rectifier/capacitor power supply project. The blue trace shows the grid voltage, slightly flattened on the peaks. The orange trace shows the primary current and the purple trace shows the secondary current. You can see that the currents are very non-sinusoidal. To correctly measure their heating effect you need a true RMS responding meter. You can see some extra waviness in the primary current compared to the secondary current; this is the exciting current that supplies the magnetic core.
Derating factors for various rectifier circuits (bridge, full wave, etc.) can be found on the web, but it's almost never explained just how these factors are determined. I'm going to show how the derating factor can be determined for a real power supply.
I will assume the project builder has a DMM capable of making "True RMS" measurements of current and voltage. You shouldn't be attempting to build a power supply without having a meter! You should also have some power resistors to use as loads. You might be able to use light bulbs, such as automobile tail light bulbs for this.
Transformers have ratings; they are designed to supply a certain maximum current at a certain secondary voltage. What determines the ratings? The answer to that question is simple; it's just a matter of how hot the transformer gets. The transformer is constructed by winding insulated copper wire around a core made of iron. The iron is in thin sheets called laminations. The copper wire is different from the wire you use to hook up parts of your circuit; it is insulated with very thin plastic-like insulation, and is known as "magnet wire". There are at least two separate windings of copper wire on the core. There is no electrical connection (also known as a "galvanic" connection) between the two coils (primary and secondary) in the type of transformers used to make our power supply; this is an important safety feature of a transformer and provides "isolation" from the grid voltage.
One particular type of transformer, a transformer which is adjustable and known as a "variac" is an auto-transformer, and does have a galvanic connection between primary and secondary. NEVER use a variac alone as the transformer in a project power supply. You may use a variac between the grid and another isolated transformer to adjust the voltage applied to the primary of the isolated transformer, but this should seldom be necessary. There are also auto-transformers that are not adjustable; they also have a galvanic connection between primary and secondary. NEVER use an auto-transformer alone as the transformer in a project power supply.
The copper wire used to make the windings has some resistance. Copper is the second best conductor of electricity (other than superconductors); that's why it's used. But its resistance is not zero, so whenever a current passes through a copper wire, the wire is heated; this heating is called "copper loss" because some of the electrical energy is lost in the process. The amount of heat generated is given by the formula P = I^2*R, where P is the power heating the wire, I is the current in the wire and R is the resistance of the wire. In texts you will find this loss referred to as "I squared R loss".
When a transformer is supplying current to a load, the primary and secondary windings get hot due to the copper loss. The primary and secondary are separated by insulation which is a special paper. If the transformer gets too hot, the plastic insulation on the magnet wire and the paper insulation will be damaged, and parts of the windings may become galvanically connected where they shouldn't be. This will result in a short circuit in the winding and could cause a fire. The manufacturer has designed the transformer so that if the rated secondary current is not exceeded, the highest temperature in the middle of the windings will not exceed a certain value. There are various classes of transformer temperature ratings. As you might expect, transformers intended for special uses, such as military use for example, are constructed to withstand higher temperatures. The typical transformer the hobbyist will use will be a class A rated transformer, with a maximum hot spot temperature of 105 degrees centigrade.
There is another source of heat in transformers. The iron core is magnetized when a voltage is applied to the primary. Since the applied voltage is AC the magnetization of the core is constantly reversing direction, 120 times a second in the U.S. Every time the magnetization is reversed, a little energy is lost and converted to heat. This is called "core loss" and its amount is dependent only on the magnitude of the voltage applied to the primary; it doesn't change noticeably with the current drawn from the secondary. Since we have no control over it, we'll ignore it; it will be a constant in our transformer.
The sort of transformers used in the project may have a center tapped secondary and the designations printed on the transformer will indicate the secondary voltage and current rating. The designation may be something like 12-0-12, or 24v CT. These two designations represent the same voltage rating, which is 24 volts AC between the outer legs of the center tapped winding, and 12 volts AC from the center tap to each of the outer legs.
To start, let's make a few measurements. I'll show the measurements I made on a transformer rated to supply 12.6 VAC at 3 amps. First measure the resistance of the primary and secondary winding. Be aware that the secondary will probably be difficult to measure accurately because its resistance will be low. Most DMMs have test leads, and the leads themselves have a resistance of a few tenths of an ohm, comparable to the resistance of the secondary winding. What you should do is to set the DMM to measure ohms and connect the ends of the test leads together; this will give you a value for the resistance of the leads (wiggle the connection of the leads and press them together with force to get a stable reading). Then connect the leads to the secondary wires of the transformer. Subtract the resistance of the leads from the reading you get on the secondary; this will be the true resistance of the secondary.
CAUTION: We need to make a measurement on the primary of the transformer while it is energized. Be very careful while doing this. You will need a line cord to plug into the wall outlet and connect this cord to the primary of the transformer. If you use "wire nuts" to make the connection, the possibility of the ends of the line cord touching will be prevented, but you can still make contact with the wire inside the wire nut with your meter probes. See here in case you don't know what a wire nut is:
http://www.bing.com/images/search?q=wire+nut&qpvt=wire+nut&FORM=IGRE
In your final version of the project, you might make soldered connections with a fuse in the primary side, all in a nice box.
EXERCISE CAUTION: Make sure the line cord is unplugged from the wall socket and connect it to the primary with wire nuts. There should be nothing connected to the secondary. Now set the DMM to measure AC volts; if the meter isn't auto-ranging, set the range to a suitable range to measure the grid voltage. Plug the line cord in so that the transformer is energized. Carefully probe into the wire nuts with the meter probes, one probe to each wire nut. This will give a reading for the grid voltage; write it down. Next, measure the voltage across the full winding of the secondary of the transformer; write this down. These two readings will allow you to calculate the turns ratio of the transformer.
The transformer primary will actually draw some current even when there is no load on the secondary. This is the current that magnetizes the core and supplies the core losses; it's called the exciting current and adds to the primary current caused by the load when the secondary is loaded.
The kind of power supply project to be built is going to be transformer based for safety reasons. It may be regulated or unregulated, but the basic circuit is a small, relatively low voltage transformer, followed by a rectifier and an electrolytic capacitor for filtering.
I'm going to be dealing with only one very specific topic, but the beginner should read this description of power supply design before continuing here:
http://www.zen22142.zen.co.uk/Design/dcpsu.htm
Beginning power supply builders soon discover that a given transformer can't supply as many DC amps when used in a power supply as the transformer is rated for by the manufacturer. This is because the transformer rating is for an AC resistive load which draws a current whose waveshape is a sine wave, like the waveform of the grid voltage. When the transformer is used in a power supply with a capacitor filter, the current drawn from the secondary is no longer a sine wave; it's a narrow, peaked waveform, and such a waveform causes extra heating in the transformer. This is why the transformer must be derated when used in a rectifier/capacitor power supply, and that's what this post is all about.
I've attached an image showing a scope capture of the voltage and currents in a rectifier/capacitor power supply project. The blue trace shows the grid voltage, slightly flattened on the peaks. The orange trace shows the primary current and the purple trace shows the secondary current. You can see that the currents are very non-sinusoidal. To correctly measure their heating effect you need a true RMS responding meter. You can see some extra waviness in the primary current compared to the secondary current; this is the exciting current that supplies the magnetic core.
Derating factors for various rectifier circuits (bridge, full wave, etc.) can be found on the web, but it's almost never explained just how these factors are determined. I'm going to show how the derating factor can be determined for a real power supply.
I will assume the project builder has a DMM capable of making "True RMS" measurements of current and voltage. You shouldn't be attempting to build a power supply without having a meter! You should also have some power resistors to use as loads. You might be able to use light bulbs, such as automobile tail light bulbs for this.
Transformers have ratings; they are designed to supply a certain maximum current at a certain secondary voltage. What determines the ratings? The answer to that question is simple; it's just a matter of how hot the transformer gets. The transformer is constructed by winding insulated copper wire around a core made of iron. The iron is in thin sheets called laminations. The copper wire is different from the wire you use to hook up parts of your circuit; it is insulated with very thin plastic-like insulation, and is known as "magnet wire". There are at least two separate windings of copper wire on the core. There is no electrical connection (also known as a "galvanic" connection) between the two coils (primary and secondary) in the type of transformers used to make our power supply; this is an important safety feature of a transformer and provides "isolation" from the grid voltage.
One particular type of transformer, a transformer which is adjustable and known as a "variac" is an auto-transformer, and does have a galvanic connection between primary and secondary. NEVER use a variac alone as the transformer in a project power supply. You may use a variac between the grid and another isolated transformer to adjust the voltage applied to the primary of the isolated transformer, but this should seldom be necessary. There are also auto-transformers that are not adjustable; they also have a galvanic connection between primary and secondary. NEVER use an auto-transformer alone as the transformer in a project power supply.
The copper wire used to make the windings has some resistance. Copper is the second best conductor of electricity (other than superconductors); that's why it's used. But its resistance is not zero, so whenever a current passes through a copper wire, the wire is heated; this heating is called "copper loss" because some of the electrical energy is lost in the process. The amount of heat generated is given by the formula P = I^2*R, where P is the power heating the wire, I is the current in the wire and R is the resistance of the wire. In texts you will find this loss referred to as "I squared R loss".
When a transformer is supplying current to a load, the primary and secondary windings get hot due to the copper loss. The primary and secondary are separated by insulation which is a special paper. If the transformer gets too hot, the plastic insulation on the magnet wire and the paper insulation will be damaged, and parts of the windings may become galvanically connected where they shouldn't be. This will result in a short circuit in the winding and could cause a fire. The manufacturer has designed the transformer so that if the rated secondary current is not exceeded, the highest temperature in the middle of the windings will not exceed a certain value. There are various classes of transformer temperature ratings. As you might expect, transformers intended for special uses, such as military use for example, are constructed to withstand higher temperatures. The typical transformer the hobbyist will use will be a class A rated transformer, with a maximum hot spot temperature of 105 degrees centigrade.
There is another source of heat in transformers. The iron core is magnetized when a voltage is applied to the primary. Since the applied voltage is AC the magnetization of the core is constantly reversing direction, 120 times a second in the U.S. Every time the magnetization is reversed, a little energy is lost and converted to heat. This is called "core loss" and its amount is dependent only on the magnitude of the voltage applied to the primary; it doesn't change noticeably with the current drawn from the secondary. Since we have no control over it, we'll ignore it; it will be a constant in our transformer.
The sort of transformers used in the project may have a center tapped secondary and the designations printed on the transformer will indicate the secondary voltage and current rating. The designation may be something like 12-0-12, or 24v CT. These two designations represent the same voltage rating, which is 24 volts AC between the outer legs of the center tapped winding, and 12 volts AC from the center tap to each of the outer legs.
To start, let's make a few measurements. I'll show the measurements I made on a transformer rated to supply 12.6 VAC at 3 amps. First measure the resistance of the primary and secondary winding. Be aware that the secondary will probably be difficult to measure accurately because its resistance will be low. Most DMMs have test leads, and the leads themselves have a resistance of a few tenths of an ohm, comparable to the resistance of the secondary winding. What you should do is to set the DMM to measure ohms and connect the ends of the test leads together; this will give you a value for the resistance of the leads (wiggle the connection of the leads and press them together with force to get a stable reading). Then connect the leads to the secondary wires of the transformer. Subtract the resistance of the leads from the reading you get on the secondary; this will be the true resistance of the secondary.
CAUTION: We need to make a measurement on the primary of the transformer while it is energized. Be very careful while doing this. You will need a line cord to plug into the wall outlet and connect this cord to the primary of the transformer. If you use "wire nuts" to make the connection, the possibility of the ends of the line cord touching will be prevented, but you can still make contact with the wire inside the wire nut with your meter probes. See here in case you don't know what a wire nut is:
http://www.bing.com/images/search?q=wire+nut&qpvt=wire+nut&FORM=IGRE
In your final version of the project, you might make soldered connections with a fuse in the primary side, all in a nice box.
EXERCISE CAUTION: Make sure the line cord is unplugged from the wall socket and connect it to the primary with wire nuts. There should be nothing connected to the secondary. Now set the DMM to measure AC volts; if the meter isn't auto-ranging, set the range to a suitable range to measure the grid voltage. Plug the line cord in so that the transformer is energized. Carefully probe into the wire nuts with the meter probes, one probe to each wire nut. This will give a reading for the grid voltage; write it down. Next, measure the voltage across the full winding of the secondary of the transformer; write this down. These two readings will allow you to calculate the turns ratio of the transformer.
The transformer primary will actually draw some current even when there is no load on the secondary. This is the current that magnetizes the core and supplies the core losses; it's called the exciting current and adds to the primary current caused by the load when the secondary is loaded.
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