Fig. 1 - A wireless charger uses induced forces to charge electrical devices without directly connecting to them
.
Induced Current Meaning
Before we get into the meaning of an induced current, we must understand the process of electromagnetic induction and how it occurs. When we have a magnetic field, one of the properties of the magnetic field is its flux. This is defined as the following.
The magnetic flux is the measure of the total amount of magnetic field strength passing through a given area.
Fig. 2 - The magnetic flux of a field passing through an area.
Due to the movement of the magnet or a reduction in the strength of the magnetic field, the magnetic flux of a magnet can change over time. This change in magnetic flux causes the phenomenon of electromagnetic induction.
Electromagnetic induction is the creation of an electromotive force (EMF) in a magnetic conductor due to an external changing magnetic flux.
Furthermore, we can also define the electromotive force in relation to potential difference as the following.
The electromotive force is how much energy is given by a power source per unit of charge passing through the circuit. It is essentially the potential difference across a power source.
This electromotive force present in the conductive material then causes current to flow, thus resulting in an induced current.
Induced Current Formula
Firstly, let's consider the formula for the magnetic flux of a field. This is given by
\[ \Phi_{\text{B}} = \int \vec{B} \cdot \mathrm{d} \vec{A} ,\]
where \( \Phi_{\text{B}} \) is the magnetic flux of a magnetic field measured in weber (\(\mathrm{Wb}\)), \(\vec{B}\) is the magnetic field vector measured in units of teslas (\(\mathrm{T}\)), and \(\mathrm{d} \vec{A}\) is the infinitesimal area vector measured in \(\mathrm{m^2}\). From the equation, the dot product highlights that we are only considering the component of the magnetic field perpendicular to the area.
Now that we have defined the magnetic flux, we can define the equation for electromagnetic induction as the following,
\[ \varepsilon = - \frac{\mathrm{d} \Phi_{\text{B}}}{\mathrm{d} t}, \]
where \(\varepsilon\) is the induced electromotive force measured in volts \(\mathrm{V}\), \(\Phi_{\text{B}}\) is the magnetic flux measured in webers \(\mathrm{Wb}\), and \(t\) is time measured in seconds \(\mathrm{s}\). This law is governed by two laws: Faraday's law and Lenz's law. The former determines the magnitude of the induced electromotive force, whilst the latter determines the direction of the induced current.
Let's consider an example where we use our electromagnetic induction formula.
Consider you have a magnet being moved alongside a metal plate made of conducting metal. The movement of the magnet generates a change in magnetic flux given by an expression \( \Phi_{\text{B}} = at^2 + bt \) where \(a\) is a constant given by a value of \(- 1.5 \, \mathrm{\frac{V}{s}} \) and \(b\) is a constant given by a value of \(-0.5 \, \mathrm{V}\). Using our formula for electromagnetic induction, how much electromotive force is induced at a time \(t = 1.2 \, \mathrm{s} \)?
To solve this, we take the time derivative of our expression for magnetic flux \(\Phi_{\text{B}}\). This results in
\[ \frac{ \mathrm{d} \Phi_{\text{B}}}{\mathrm{d} t} = 2at + b .\]
Plugging this expression into the electromagnetic induction equation, we find
\[ \begin{align} \varepsilon &= - \frac{\mathrm{d} \Phi_{\text{B}}}{\mathrm{d} t} \\ \varepsilon &= - 2at - b . \end{align} \]
Finally, we can substitute the time value and our constants to find
\[ \begin{align} \varepsilon &= - \frac{\mathrm{d} \Phi_{\text{B}}}{\mathrm{d} t}|_{t = 1.2 \, \mathrm{s}} \\ \varepsilon &= -(2 \times -1.5 \, \mathrm{\frac{V}{s}} \times 1.2 \, \mathrm{s} ) - (-0.5 \, \mathrm{V} ) \\ \varepsilon &= 4.1 \, \mathrm{V} . \end{align} \]
Direction of Induced Current
As we mentioned briefly earlier, the direction of the induced electromotive force in electromagnetic induction is determined using Lenz's law.
Lenz's law states that the direction of an induced current will always be flowing in such a direction that it will oppose the motion causing it.
Fig. 3 - When the magnet enters the tube, it experiences an upward force due to Lenz's law.Referring to the figure above, let's consider a magnet being dropped through a tube made of conducting material. As the magnet falls, there is an induced current in the aluminum material. As current runs through it, the tube itself generates its own magnetic field. However, this time, the direction of the magnetic field is opposite in direction to that of the magnet falling through the tube. To determine whether the current flowing in the tube is clockwise or anticlockwise, we can use the right-hand rule.
To use this method, curl the fingers on your right hand as if you are enclosing a tube. The direction of your fingers should follow the direction of the induced current. Then extend out your thumb; the direction your thumb is pointing indicates the north pole of the conductor, as the current has essentially turned the conductor into a magnet. Since we know that the conductor must repel the falling magnet, this means that the north pole of the conductor must be pointing upwards to repel the falling magnet with a like pole. Pointing our thumb upwards, we find that the resultant curl of our fingers is in the counter-clockwise direction, which is the direction of the induced current in the tube. This repels the north pole of the magnet from being dropped into the tube, thus creating an opposing force that reduces the acceleration.
The right-hand grip rule can also be used to determine the direction of the magnetic field generated by a current running through a wire. In this case, the thumb points in the direction of the current, whilst the direction of your fingers indicate the curvature of the generated magnetic field.
Difference between Current and Induced Current
Normal current occurs when we have a typical circuit set-up with a power source connected to a resistor. Referring to the figure below, we have a connected circuit with conventional current \(I\) flowing through the resistors due to the power source.
Fig. 5 - A standard circuit set-up with conventional current flowing through the components and the wires.
On the other hand, an induced current is generated from an external changing magnetic flux. As we saw earlier, examples of induced current can occur when a magnet falls through a conductive tube or a magnet moves next to a conductive material. Examples of the applications of inductive current are seen in wireless chargers and induction stoves.
Geomagnetically Induced Currents
A large-scale example of induced forces is geomagnetically induced currents, also referred to as GICs. Just like how magnets have their own surrounding magnetic fields, our Earth also has an enormous magnetic field surrounding the globe. This field is generated by the convection of radioactive heating at our Earth's core. Thus, our North pole and South pole behave exactly like the north and south poles of a magnet.
Geomagnetically induced currents are currents induced in the surface of the Earth due to the change in the Earth's surrounding magnetic fields.
Changes in the Earth's surrounding magnetic field are caused by space weather events such as solar wind. Fluctuations in the field behave like a moving magnet, changing the flux of the magnetic field over time. Thus any conductive material on the surface of the Earth, such as gridlines or pipelines, will have a current induced in them as a result of the changing field. This can negatively affect the machinery and cause damage to electrical transmissions.
Induced Currents - Key takeaways
- The magnetic flux is the measure of the total amount of magnetic field strength passing through a given area.
- Electromagnetic induction is the creation of an electromotive force (EMF) in a magnetic conductor due to an external changing magnetic flux.
- The electromagnetic induction equation is given by \( \varepsilon = - \frac{\mathrm{d} \Phi_{\text{B}}}{\mathrm{d} t} \).
- The direction of the induced current can be determined using the right-hand rule.
- Conventional currents flow in circuits from a power source, whereas the induced current is generated by a changing external magnetic field.
- Geomagnetically induced currents are a result of the Earth's changing magnetic field.
References
- Fig. 1 - Wireless charger, flickr.com (https://flickr.com/photos/honou/22063888805/in/photolist-zBHcrX-27ruXUs-K7rg6v-26eRVX3-N4VqKN-2fK1mVq-LrobZ6-2a85Edu-244pnjn-296UpVC-296UpPW-LrocLM-Lroaci-2m9adNJ-N4VsKQ-27ruXxq-N4Vozq-2acpu5k-2hH5uNC-Lro9CH-2acpufv-241tagf-LrobvR-N4VsSo-24zVqcW-2dgxWtx-Lrobcz-EpczyX-2a85DVL-N4Vsy7-EpcA1t-241t7CE-FVqnxu-244ps9c-EpczNV-241tc1N-241tbR9-241t8my-FVqnbY-KcHXJb-Lroa1B-N4Vre3-241t7Uw-EpcAEz-241tctb-KcHVPu-241ta91-241tbdL-2dUnf7t-7YNd6k) Licensed by CC BY 2.0 (https://creativecommons.org/licenses/by/2.0/)
- Fig. 2 - Magnetic flux, StudySmarter Originals.
- Fig. 3 - Magnet falling inside tube, StudySmarter Originals.
- Fig. 4 - Right-hand rule, StudySmarter Originals.
- Fig. 5 - Electrical circuit, StudySmarter Originals.
- Fig. 6 - Earth's magnetic field, StudySmarter Originals.
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