Edexcel Physics A-level Topic 7: Electric and Magnetic Fields

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Comprehensive vocabulary flashcards covering electric fields, capacitance, magnetism, and electromagnetic induction based on A-level Physics notes.

Last updated 10:02 PM on 5/13/26
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44 Terms

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Force field

An area in which an object experiences a non-contact force, represented as vectors (which describe the direction of the force that would be exerted on the object and from this you can deduce direction of field) or diagrams containing field lines. The distance between field lines represents the strength of the force exerted by the field in that region.

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Electric field

A force field in which charged particles experience a force.

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Electric field strength (EE)

The force per unit charge experienced by an object in an electric field, given by the formula E=FQE = \frac{F}{Q}, where FF is force and QQ is charge. This value is constant in a uniform field but varies in a radial field.

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Coulomb’s law

A law stating that the magnitude of the force between two point charges is directly proportional to the product of their charges and inversely proportional to the square of the distance between them: F=Q1Q24πϵ0r2F=\frac{Q_1Q_2}{4\pi\epsilon_0r^2} . Epsilon is the permittivity of free space, Q1/Q2 are charges and r is the distance between the charges.

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Permittivity of free space (ϵ0\epsilon_0)

A physical constant used in the calculation of electric force and potential in a vacuum.

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Charges have the same sign

So force will be repulsive, if charges have different signs the force will be attractive.

<p>So force will be repulsive, if charges have different signs the force will be attractive.</p>
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Point charges

Form a radial electric field, can calculate electric field using formula E=Q4πϵ0r2E=\frac{Q}{4\pi\epsilon_0r^2}

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Absolute electric potential (VV)

The potential energy per unit charge of a positive point charge at a specific point in a field; it is zero at infinity.

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Absolute magnitude of electric potential

Greatest at the surface of charge and as the distance from the charge increases the potential decreases so electric potential at infinity is zero.

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Electric potential difference (ΔV\Delta V)

The energy needed to move a unit charge between two points. Whether the value of potential is negative or positive depends on the sign of the charge (Q).

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When electric potential is

Positive: Charge is positive, and charge is repulsive Negative: charge is negative and the force is attractive

<p>Positive: Charge is positive, and charge is repulsive Negative: charge is negative and the force is attractive</p>
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Electric fields between parallel plates

Uniform electric field. Calculate Electric field strength (E) in electric field formed between parallel plates by using E=VdE=\frac{V}{d}

<p>Uniform electric field. Calculate Electric field strength (E) in electric field formed between parallel plates by using $$E=\frac{V}{d}$$ </p>
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Electric potential in a radial field

To find the electric potential in a radial field use formula V=Q4πϵ0rV=\frac{Q}{4\pi\epsilon_0r} , ϵ0\epsilon_0 is the permitivitty of free space, Q is the charge, r is the distance between the charges.

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Electric field types

uniform or radial

<p>uniform or radial</p>
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Uniform electric field

Exerts the same electric force everywhere in the field, has parallel and equally spaced field lines, distance between field lines represent magnitude of force (field lines are at the same distance so stays the same throughout). Equipotential surfaces are planes which are equally spaced and parallel to the plates.

<p>Exerts the same electric force everywhere in the field, has parallel and equally spaced field lines, distance between field lines represent magnitude of force (field lines are at the same distance so stays the same throughout). Equipotential surfaces are planes which are equally spaced and parallel to the plates.</p>
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Radial electric field

Magnitude of electric force depends on the distance between the two charges (e.g as charge moves further away from the centre. The magnitude of force would decrease as distance between field lines increases), equipotential surfaces around point charge for concentric circles.

<p>Magnitude of electric force depends on the distance between the two charges (e.g as charge moves further away from the centre. The magnitude of force would decrease as distance between field lines increases), equipotential surfaces around point charge for concentric circles.</p>
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Equipotential surface

A surface where the potential is the same everywhere; consequently, no work is done when a charge moves along it.

<p>A surface where the potential is the same everywhere; consequently, no work is done when a charge moves along it.</p>
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Capacitance (CC)

The charge stored by a capacitor per unit potential difference, defined by the formula C=QVC = \frac{Q}{V}.

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Electrical energy stored by a capacitor (WW)

Represented by the area under a graph of charge against potential difference, calculated as W=12VQW = \frac{1}{2}VQ, W=12CV2W = \frac{1}{2}CV^2, or W=Q22CW = \frac{Q^2}{2C}.

<p>Represented by the area under a graph of charge against potential difference, calculated as $$W = \frac{1}{2}VQ$$, $$W = \frac{1}{2}CV^2$$, or $$W = \frac{Q^2}{2C}$$.</p>
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Capacitor charging

Current starts to flow and negative charge builds up on the plate connected to the negative terminal. On the opposite plate electrons are repelled by the negative charge building up on the initial plate, therefore these electrons move to the positive terminal and equal and opposite charge formed on each plate creating potential difference. As charge across plates increases, pd increases but electron flow decreases due to force of electrostatic repulsion also increasing therefore current decreases and eventually reaches zero.

<p>Current starts to flow and negative charge builds up on the plate connected to the negative terminal. On the opposite plate electrons are repelled by the negative charge building up on the initial plate, therefore these electrons move to the positive terminal and equal and opposite charge formed on each plate creating potential difference. As charge across plates increases, pd increases but electron flow decreases due to force of electrostatic repulsion also increasing therefore current decreases and eventually reaches zero.</p>
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How to charge a capacitor

Connect it in a circuit wit power supply and resistor

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How to discharge a capacitor

Connect it in a closed circuit with just a resistor

<p>Connect it in a closed circuit with just a resistor</p>
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Capacitor discharging

When capacitor is discharging the current flows in the opposite direction and current charge and potential difference across the capacitive will all fall exponentially meaning it will take same amount of time for each of the values to halve.

<p>When capacitor is discharging the current flows in the opposite direction and current charge and potential difference across the capacitive will all fall exponentially meaning it will take same amount of time for each of the values to halve.</p>
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Time constant (RCRC)

The product of resistance and capacitance, representing the time taken to discharge a capacitor to 0.370.37 (e1e^{-1}) of its initial value or charge it to 0.630.63 (1e11 - e^{-1}) of its maximum value. Can be calculated by finding time where values are 0.37 of initial value if discharging or 0.63 of the maximum value if charging

<p>The product of resistance and capacitance, representing the time taken to discharge a capacitor to $$0.37$$ ($$e^{-1}$$) of its initial value or charge it to $$0.63$$ ($$1 - e^{-1}$$) of its maximum value. Can be calculated by finding time where values are 0.37 of initial value if discharging or 0.63 of the maximum value if charging</p>
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Gradient of ln(Q) against t

Gradient of graph is 1RC\frac{-1}{RC}. Therefore RC=1gradientRC=\frac{-1}{gradient}

<p>Gradient of graph is $$\frac{-1}{RC}$$. Therefore $$RC=\frac{-1}{gradient}$$ </p>
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Magnetic flux density (BB)

A measure of the strength of a magnetic field, measured in Tesla (TT).

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Magnetic flux (ϕ\phi)

A value describing the magnetic field lines passing through a given area, calculated by Φ=BA\Phi = BA when the field is perpendicular to the area.

<p>A value describing the magnetic field lines passing through a given area, calculated by $$\Phi = BA$$ when the field is perpendicular to the area.</p>
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Magnetic flux linkage (NΦN\Phi )

The magnetic flux multiplied by the number of turns (NN) of a coil, given by NΦ=BANN\Phi=BAN . B is magnetic flux density, A is the area and N is the number of turns.

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Charged particles moving in a magnetic field

Force acts on charged particles moving in a magnetic field. Reason why force exerted on current carrying wire in a magnetic field because it contains moving electrons which are negatively charged. Magnitude of force calculated as F=BQvsinθF=BQv\sin\theta . B is magnetic flux density, Q is charge and v is velocity of particle.

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Fleming’s left hand rule

Used to find direction of force exerted on a charged particle where the thuMb represents Motion/force, the First finger represents Field, and the seCond finger represents Conventional Current (opposite direction to electron flow) Use second finger as the direction of travel, however if the charge on the particle is negative reverse the direction of your second finger because conventional current flows from positive to negative. Force causes charged particles to follow a circular path when in a magnetic field and acts as centripetal force

<p>Used to find direction of force exerted on a charged particle where the thu<strong>M</strong>b represents Motion/force, the <strong>F</strong>irst finger represents Field, and the se<strong>C</strong>ond finger represents Conventional Current (opposite direction to electron flow) Use second finger as the direction of travel, however if the charge on the particle is negative reverse the direction of your second finger because conventional current flows from positive to negative. Force causes charged particles to follow a circular path when in a magnetic field and acts as centripetal force</p>
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Current carrying conductors in a magnetic field

When current passes through a wire, magnetic field is induced (this is true for any long straight current carrying conductor) Field lines of the induced magnetic field form concentric rings around the wire

<p>When current passes through a wire, magnetic field is induced (this is true for any long straight current carrying conductor) Field lines of the induced magnetic field form concentric rings around the wire</p>
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Current carrying wire in a magnetic field force

Magnitude of force found by F=BIlsinθF=BIl\sin\theta , B is magnetic flux density I is current and l is they length of the wire in the magnetic field. Direction using Flemings left hand rule.

<p>Magnitude of force found by $$F=BIl\sin\theta$$ , B is magnetic flux density I is current and l is they length of the wire in the magnetic field. Direction using Flemings left hand rule.</p>
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Electromagnetic induction

The phenomenon where an emf is induced in a conductor when it moves relative to a magnetic field, electrons in the rod will experience a force and build up on one side. Or if magnet moves relative to a coil of wire. If the coil forms a complete circuit, current is also induced.

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Faraday’s law

A law stating that the magnitude of induced emf (ϵ\epsilon ) is equal to the rate of change of flux linkage: ϵ=NΔΦΔt\epsilon=\frac{N\Delta\Phi}{\Delta t} . Measures the rate of change of flux linkage

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Lenz’s law

A law stating that the direction of induced current is such as to oppose the motion causing it, which is a direct consequence of the conservation of energy.

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Mutual inductance

A process where a change in current in one coil induces an emf in a second coil located within the first coil's magnetic field. The induced emf in the second coil is proportional to to the change in current in the first coil. E.g transformer

<p>A process where a change in current in one coil induces an emf in a second coil located within the first coil's magnetic field. The induced emf in the second coil is proportional to to the change in current in the first coil. E.g transformer</p>
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Demonstrate Lenz’s law

Measure the speed of a magnet falling through a coil of wire and its speed when falling from the same height without falling through the coil. Magnet takes longer to reach the ground when it moves through the coil. 1. As magnet approaches copil change in flux through the coil so emf and current induced 2. Due to Lenz’s law the direction of induced current is such as to oppose the motion of the magnet so the same pole as pole of magnet approaching coil is induced in order to repel the magnet. Causes magnet to slow down due to electrostatic forces of repulsion. 3. As the magnet passes through the centre of the coil there is no change in flux so no emf is induced 4. Magnet begins to leave coil, change in flux so current induced opposing motion of magnet. Opposite pole induced by magnet causing it to slow down once again due to electrostatic forces of attraction.

<p>Measure the speed of a magnet falling through a coil of wire and its speed when falling from the same height without falling through the coil. Magnet takes longer to reach the ground when it moves through the coil. 1. As magnet approaches copil change in flux through the coil so emf and current induced 2. Due to Lenz’s law the direction of induced current is such as to oppose the motion of the magnet so the same pole as pole of magnet approaching coil is induced in order to repel the magnet. Causes magnet to slow down due to electrostatic forces of repulsion. 3. As the magnet passes through the centre of the coil there is no change in flux so no emf is induced 4. Magnet begins to leave coil, change in flux so current induced opposing motion of magnet. Opposite pole induced by magnet causing it to slow down once again due to electrostatic forces of attraction. </p>
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Faraday and Lenz law combined

ϵ=Δ(NΦ)Δt\epsilon=\frac{-\Delta\left(N\Phi)\right.}{\Delta t}

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Peak value (1)

Maximum value (amplitude)

<p>Maximum value (amplitude)</p>
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Root mean square (2)

Average of all the squares of the possible values this value give you the effective value of current/voltage output

<p>Average of all the squares of the possible values this value give you the effective value of current/voltage output</p>
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Time period (4)

Time taken to complete one full cycle.

<p>Time taken to complete one full cycle.</p>
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Frequency

Number of complete oscillations passing through a point per second

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Root mean square (rms) value

The effective value of an alternating current or voltage, calculated as the average of all the squares of the possible values; for sine waves, Vrms=V02V_{rms}=\frac{V_0}{\sqrt2} . Irms=I02I_{rms}=\frac{I_0}{\sqrt2} , I0I_0 is peak current and V0V_0 Is peak voltage

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UK Mains Voltage

The electricity supplied to homes in the UK, which has an rms voltage value of around 230V230\,V.