Home
Anatomical Models
Biology
Chemistry
Physics
Mechanics
Electricity
Compass
Counters
DC Motors
Glassware
Gyroscope
Hygrometer
Light (Optics)
Lab Supplies
Labware
Magnets
Metals
Microscopes
Multi-meters
pH meters
pH Papers
Pulleys
Levers
Refractometers
Scales
Thermometers
Tools

Please select from the list below or the links on the right. 

Primary and Secondary Coil Set

Learning about Transformers and how they work

Introduction: The primary & secondary coil with a center core is basically a transformer. A transformer is an electrical device without any moving components that consists essentially of two electrical circuits interlinked with a magnetic field.

The function of the transformer is to transform electric power from low voltage and large current to high voltage and low current, or the reverse.

Transformers can be fun, useful and dangerous. Caution should be used. Some transformers are capable of producing enough voltage to kill a person.

The input circuit or winding of the transformer is called the primary, and the output circuit the secondary. The primary and secondary coil can be used to either step up or down (increase or decrease) the voltage or current.

Power is a measurement that is derived by multiplying the voltage (in volts) times the current (in amps).

A transformer does not create power. So if the voltage increases, the current will go down. If the voltage is decreased, the current will be increased. The power will always stay the same.

Example:
If the voltage is 20 volts and the current is 2 amps, you may use a transformer to cut the voltage in half, then the current would double. In other words the voltage would become 10 and the current would become 4 amps.

20 volts x 2 amps = 40 watts and 10 volts x 4 amps = 40 watts.

As you see a transformer can change the voltage and current, but the power remains the same.

How Transformers Work?

When an alternating current flows through a conductor, an alternating magnetic field is generated around the conductor. This alternating magnetic field can induce an alternating current in any conductor or coil that is close to it.

In a transformer, one of the coils (known as input or primary) receives the electricity and produces a magnetic field and the other coil (known as output or secondary) absorbs that magnetic energy and converts it to electrical energy.

These coils are usually wrapped around the same core. For power transformers this core is most often made of iron. Other types of transformers may use other material or no core at all. In order for a transformer to work the incoming current must be fluctuating. That is turning on and off or higher and lower. Generally this fluctuating current is provided by AC power. AC stands for alternating current. AC is constantly alternating from positive to negative.

As AC passes through a coil that surrounds an iron core, a varying electromagnetic field is created around the coil and in the core. This electromagnetic field then induces a second current in the second coil or coils. This is referred to as induced voltage. The first coil in which the current is supplied is known as the primary coil, and the coil with induced voltage is known as the secondary coil.

The relation of secondary voltage to the primary voltage in a transformer equals to the relation of windings on the secondary coil to the windings of the primary coil.

If the secondary coil has twice as many turns as the primary then the induced voltage on the secondary coil will be twice as high. If the secondary coil has half as many windings as the primary then the voltage on the secondary coil will be half as much.

Remember, however, that if the voltage is cut in half the amperage doubles.

Direct current cannot transfer power by means of a transformer because it does not generate a changing magnetic field. However, DC voltages can be made to pulsate on and off to induce a changing magnetic field. This acts almost the same as AC current.
The primary winding receives electrical energy from a power source and couples this energy to the secondary winding by means of changing magnetic field. The energy appears as an EMF across the secondary winding, and if a load is connected to the secondary, the energy is transferred to the load. A transformer does not generate electrical power, but merely transfers it.

The primary circuit draws the power from the source, the secondary delivers the power to the load. The power transferred from the primary to the secondary is determined by the current flowing in the secondary, which in turn, depends on the power required by the load. In an ideal transformer the power in the primary circuit equals the power in the secondary circuit. Since power is voltage times current or:

Vp x Ip = Vs x Is

Primary Voltage x Primary Current = Secondary Voltage x Secondary Current

when the primary and secondary voltages are equal, as in a case of transformer with equal number of turns in primary and secondary, the primary current will automatically adjust to the same value as the secondary current so that the primary and secondary powers are equal.

 

Transformer uses

Transformers are used by the power companies for a very good reason. Voltage is stepped up to as high as 70,000 volts before it is transmitted across the power lines. This is done for two important reason.

  1. Low voltage require much thicker cables resulting a dramatic increase on the cost of wires and installations.

  2. Low voltage electricity is lost through the wires much easier than higher voltage. This is known as line loss.

After the electricity reaches its destination it is once again stepped back down.
However, transformers are not only used to step voltage up or down, they are also used to isolate different parts of an electrical circuit from each other because they can allow AC current but block DC current.

Transformer Experiments

As with any electrical device, normal safety precautions against physical contact with powered circuits should be exercised. Since secondary design criteria for the Transformer is maximization of efficiency and in use durability, coil and core components provided exceed construction requirements for operation at the recommended voltage range. However, as a matter of policy the following safety condition should be adhered to:

DO NOT OPERATE THE TRANSFORMER IF CALCULATED VOLTAGE AT THE SECONDARY EXCEEDS 24 VRMS.

In order to experiment with the coil you will need some type of AC or a pulsating DC power source. You also need a voltmeter or multimeter that measures volts. Hook up the meter to the secondary post. If you do not have an AC power source you can briefly touch the low side of the transformer with a DC source and witness a quick flash of reading on a DC voltmeter hooked to the other side. This will only last for an instant but it will demonstrate how the sudden fluctuation through the coil will produce voltage in the other coil.

If you will apply a small AC voltage (i.e. 2 volt) to a transformer primary of 30 windings, you should get a reading of 18 volts on the other side if the transformer’s secondary has 270 windings. That is because there is a 9 to 1 ratio between the number of turns of wire on each side. Therefore 2v. x 9 = 18 volts. If you reverse the connections so that the 2 volts is on the high side and took a reading of the other side you should get a reading in the vicinity of .22 volts. 2 / 9 = .2222. Again about a 1 to 9 ratio.

Try this for several different voltages but please keep your inputs low because stepping up voltage like this can become very dangerous. Even with pulsating DC you can get a pretty good shock if too much is applied to the low side.

BASIC TRANSFORMER EXPERIMENTS

PLEASE NOTE * A VARIABLE POWER SOURCE IS RECOMMENDED FOR
THESE EXPERIMENTS.

YOU MAY USE ANOTHER TRANSFORMER TO CREATE LOW VOLTAGE AC CURRENT FOR YOUR EXPERIMENTS

1. Insert the steel rod into the plastic tube, and have the students push it back and forth to see that it moves freely when there is no current applied to the coil.

2. Apply power to the coil and have the students push the steel rod slightly out of position. Notice that the magnetic field has induced a magnetic field in the steel rod which is related to the magnetic field of the coil, and that the rod is drawn back to a centered position.

3. Attach an ammeter between one of the power leads and the coil. Measure the current draw when the coil and the steel rod are in equilibrium.

4. With the ammeter still in place, move the steel rod out of the center position. Is there an increase in the resistance of the coil?

5. Slowly increase the current supplied to the coil. Does the movement of the steel rod change as the current is increased? What does this say about the strength of the magnetic field.

(NOTE: When the coil is being held vertically, as the magnetic field increases in strength the steel rod should move more freely, to the point where the strength of the magnetic field will counterbalance the gravitational force acting on the rod. At this point the rod should "float" in the center of the plastic tube).

INCREASE THE CURRENT SLOWLY, BEING CAREFUL NOT TO EXCEED SAFE LIMITS. OBSERVE THE COIL CLOSELY FOR SIGNS OF HEATING.

ADVANCED TRANSFORMER EXPERIMENTS

1. Carefully weigh the steel bar.

2. Adjust the current to the coil to the point where the rod is just "floating".

3. Using the weight of the rod, and the current required to counteract the Earth's gravitational field, calculate the strength of the gravitational field (OR use the strength of an unknown magnetic field). This is a difficult calculation, and is only to be used for advanced studies.

4. Knowing the size of the coil, is it possible to calculate the resistance of the wire used in the apparatus? (HINT: measure the resistance of the coil, using an ammeter, both with and without the steel rod in place).
It may be pointed out that the principles involved in this apparatus are the same as are used for such applications as automotive starters, door bells, and switches.

The suggestions for the use of this apparatus are designed to show some of the possible uses. There are many other applications which the individual instructor may find useful, and which may be adapted to serve the instructional needs of a particular curriculum. The instructor should feel free to experiment with this apparatus, ALWAYS REMAINING AWARE OF PROPER SAFETY CONSIDERATIONS.

TRANSFORMER VOLTAGE: The voltage induced in a coil is equal to the sum of the many voltages induced in each loop that the flux lines cut.
Assuming that all of the magnetic flux lines pass through both windings, then, in an ideal transformer, the voltage induced in the secondary will depend on the ratio of the number of turns in the secondary winding to the number of turns in the primary winding. This exact relationship in an ideal transformer between the primary and secondary voltages (V) and their number of turns (N) can be summarized by following equations:

Vp      Np              Primary Voltage               Primary Windings
---- = ----    OR   --------------------    =   --------------------
Vs       Ns            Secondary Voltage           Secondary Windings

also Vp/Np = Vs/Ns or Vp/Vs = Np/Ns

Therefore, the secondary voltage is equal to: Vs = Vp (Ns/Np)

For example, if 12 volts is applied to a step-down transformer with 200 turns in the primary winding and 100 turns in the secondary winding, then to find the voltage of the secondary circuit:

Vs = Vp (Ns/Np) = 12V (100/200)
Vs = 6 volts

If the same transformer was used in the step up mode with 12 volts applied to the primary circuit having 100 turns, then the voltage in the secondary would be:
Vs = Vp (Ns/Np) = 12V (200/100)
Vs = 24 volts

TRANSFORMER CURRENT: A transformer does not generate power - it transfers power from the primary coil to the secondary coil. If we assume an ideal transformer then the power in the primary is equal to power in the secondary or, Vp x Ip = Vs x Is

Ideal transformer is a transformer that does not loose any power/ energy in the form of heat.

Since turn ratio determines the relationship between primary and secondary voltages, turn ratio relationship must exist between primary and secondary current.

From the power equation it is evident that voltages and current are inversely proportional to each other. For power in the primary to equal to that in the secondary, as voltages increase in the secondary currents must decrease and vice versa. If the number of turns in the secondary directly govern voltage increase or decrease between primary and secondary, turn ratio between the primary and secondary will inversely govern currents in primary and secondary.

Ip x Np = Is x Ns  or  Is/Ip = Np/Ns

and the respective currents will equal to,

Ip = Is (Ns/Np) and Is = Ip (Np/Ns)

For example: In the step-down mode, if the primary (N=200) circuit voltage is 12 volts and the current is 4 amps and the secondary (N=100) circuit voltage is 6 volts - current in the secondary will equal:
Is = (VpIp) /Vs = Ip (Np/Ns)
Is= (12Vx4A)/6V = 4A (200/100)
Is= 2 x 4A = 4A x (2)
Is= 8A

Current will flow in the secondary circuit only when a load is attached to the winding. When no current is drawn from the secondary, i.e. the circuit is open, the resistance to current flow set up by self-induced voltage or counter EMF (electromotive force) in the primary winding permits practically no current flow in that circuit. However, when a load (such as a resistor) is attached to the secondary winding and current is drawn, the counter EMF in the primary is reduced resulting in increased current flow in that circuit. The primary current will increase until the self-induced EMF will balance the induced EMF of the secondary circuit. Thus the self-induced EMF in the primary and hence the current in that circuit- will be regulated by the current drawn in the secondary circuit.
When an AC voltage is applied across a resistance, an AC current flows through the resistance. The magnitude of the current at any instant is directly proportional to the magnitude of the voltage at that instant, and is inversely proportional to the value of the resistance. This is the same relationship that exists between the current, voltage and resistance in DC circuit, and so, in AC circuit that contains only resistance, the relationship between the current, voltage and resistance is that of Ohm's Law. I = V/R

Several examples will help illustrate how we can use Ohm's Law to find magnitude of current flow in transformer circuits.

STEP-DOWN TRANSFORMER
PRIMARY SECONDARY
Secondary current: Is = Vs/Rs = 6 V/10 = 0.6A
Primary current:  Ip = (Vs / Vp) x Is = (6V/12V) 0.6A = 0.3A

STEP-UP TRANSFORMER
PRIMARY SECONDARY
Secondary current: Is = Vs / Rs = 24 V / 10 = 2.4 A
Primary current: Ip = (Vs / Vp) x Is = (24V/12V) 2.4 A = 4.8 A

TRANSFORMER EFFICIENCY: Ideally transformers should operate without loss of power during operation; that is, they should transfer 100% of the power from the primary to the secondary circuit. In any practical transformer, the output power is less than the input power so the efficiency is less than 100%. Actual losses do occur, principally through ohmic heating of the copper windings, flux leakage, and core losses due to eddy currents, hysteresis and saturation loss within the core.

Mathematically, the efficiency of a transformer is equal to the output (secondary) power divided by the input (primary) power.

OHMIC AND FLUX LOSSES: Transformer windings are usually made of many turns of copper wire. As with any wire, these windings have resistance. The longer the effective length of the wire (number of turns) and the smaller the cross sectional area of the wire, the greater is the resistance. When the primary and secondary currents flow through the windings, power is dissipated in the form of heat. These power losses are proportional to the square of the current and to the resistance. The total ohmic power loss for a transformer is equal to the sum of the losses in the primary and secondary coils. Or

Ohmic Power Loss = Ip2 Rp + Is2 Rs

where the Rp and Rs are the resistances of the primary and secondary windings respectively.

A source of inefficiency in iron-core transformers results from the fact that not all of the flux lines produced by the primary and secondary windings travel through the iron core. Any flux lines that leak from the windings into space and do not link the primary and secondary windings represent wasted energy and thus transformer power loss.

HYSTERESIS LOSS: Hysteresis loss in a transformer depends on the core material used. In an iron-core transformer, the core is magnetized by the magnetic field created by the current through the windings. The direction in which the core is magnetized is the same as the direction of the magnetic field that causes the core to be magnetized. Thus, each time the magnetic field around the windings expands and collapses, the direction in which the core is magnetized also changes. When the magnetic field collapses not all of the core material molecules assume the random orientation of unmagnetized state. As the magnetic field reverses direction, additional energy is required to orient these molecules in the direction of the magnetic field. This energy is the hysteresis loss of the transformer.

EDDY CURRENT LOSSES: The core material is made of a material that enhances the magnetic field generated when current is flowing through the windings. However, this material is also a fair conductor of electricity. Thus, the magnetic field that induces a voltage potential in the core material resulting in current flow there as well. These induced currents are called eddy currents. They produce heat and thus use energy that would otherwise be transferred to the secondary winding.
To reduce eddy currents, the core of a transformer is usually made up of many thin sheets laminated or insulated with varnish in a direction perpendicular to that which the eddy currents would tend to flow. The cross section of each current path is reduced and the resistance to eddy current flow is increased.

When the current in the primary of an iron core transformer increases, the flux lines generated follow a path through the core to the secondary winding and back through the core to the primary winding. As the current begins to increase, the number of flux lines increases rapidly. The more current rises the greater is the number of flux lines within the core until the current has risen to the point where additional rise produces relatively few additional flux lines. At this point the core is said to be saturated. Any further increase in primary current after core saturation has been reached results in wasted power, since the magnetic field cannot couple the additional power to the secondary.

Solid Core: Eddy current flow is appreciable.

Laminated Core: Cross section of currents reduced, resistance increased. Eddy current losses reduced.

TRANSFORMER CONSTRUCTION: Commercial transformers of the type commonly used in electrical devices are constructed to keep leakage of magnetic flux to a minimum. In an iron core transformer, the laminated core segments are bound together very tightly to reduce flux loss and to eliminate a possible 60 Hz hum that might develop from loose core segments. Power transfer efficiencies in the range of 95% to 99% are typical for well-constructed commercial transformer.

Educational transformers (Primary Secondary Coil Set)

Experimental Transformer for studying electromagnetic induction, ferromagnetism and principles of a transformer. Consists of two coils wound with enameled copper wire over heavy plastic spools fitting one within the other. Both coils are equipped with binding posts and a soft iron core for induction studies.

Product Code: GS1440

 Used to study electromagnetic induction & transformer principles. Overall height is at least 82 mm.

Experimental transformers may be made in different sizes, but they all serve the same functions. All coils are wrapped with magnet wire with insulated binding posts as connectors. Either coil may be used as primary or secondary. Advanced users may modify the effective number of windings on the outer coil by tapping in wire or adding to the windings.

Price and availability

* Ideal transformer is a transformer that does not loose any power in the form of heat.

Distributors of scientific and educational products

Where to buy?

Most pictures are linked to the pricing and online store for fast and convenient ordering

Our products are available at the following online stores. For large orders please call in advance and verify the availability, wholesale discounts and shipping options. If you cannot find any product in the online store of your choice, please use the search option of the store or call (973)777-3113 for further assistance.

SchoolOrders.com
MiniScience
CanadaScientific
ScienceKitStore
ChemicalStore
ScienceProjectStore

  All orders will be shipped from our warehouses in United States (USA), Canada or United Kingdom. We ship worldwide to most countries including U.S., Canada, Australia, United Kingdom, New Zealand, Germany, France, Netherlands, and many other countries.

List of metals for science experiments

Multimeters

Miniature Light Bulb
Miniature Light Bulbs
Miniature Lamp holder
Miniature Lamp Holders

Metal lamp holders

Test Leads

Plastic Battery Holders

Buzzer, 3-V DC

Crystal Earphone
Simple Switch, Knife Switch
Simple Switch

 

Transformer
Transformers
Banana Jack
Banana Jacks
banana Plug
Banana Plugs
Binding Post
Binding Posts
Dynamo, Bicycle Generator
Dynamo, Generator
Electric Bell
Bells and Buzzers
Magnet Wire
Magnet Wire
Transformer Coil, Educational
Transformer Kit

Knife Switch with plastic screw connectors

Electromagnet
Wire
Wires

UV Lamp/Fixture

Thermoelectric Cooler
Battery Holder, Metal, D Size
Metal Battery Holders

Thermoelectric Generator

Portable UV light (Blacklight)

Push Button Switches

Subminiature light bulbs

 

Copyright 2005 MiniScience Inc.