Electricity (2) Flashcards

1
Q

Capacitors

A

Capacitors:

  • Store energy in circuits by storing electric charge, creating electric potential energy.
  • Consist of two conductive plates separated by a dielectric, preventing charge flow.

===

Parallel Plate Capacitor:

  • Q: Charge stored on the plates.
  • V: Potential difference across the plates.
  • One plate holds +Q, the other –Q, with a potential difference V between them.
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2
Q

Capacitance

A

Capacitance:

  • Defined as the charge stored per unit potential difference.
  • Units: Farads (F), often in smaller units like μF, nF, or pF.

===

Capacitance Equation:

  • C = Q / V where:
    • C = capacitance.
    • Q = charge stored.
    • V = potential difference.

===

Key Points:

  • Charge stored refers to the magnitude of charge on each plate or surface of a spherical conductor.
  • Higher capacitance means the capacitor can store more charge for the same potential difference.
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3
Q

Use of capacitors

A
  • Energy storage: Capacitors store electric potential energy for various applications.
  • Camera flashes: Provide a bright flash of light during discharge.
  • Smoothing currents: Stabilize current in electronic circuits.
  • Backup power: Supply power during unexpected outages for memory devices like calculators.
  • Timing circuits: Used in electronic timers for precise operations.
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4
Q

Charging capacitor

A
  1. Initial Setup:
    • A circuit with a battery (e.m.f. ε), resistor (R), capacitor (C), and switch connected in series.
  2. Switch Closed:
    • Electrons flow from the negative terminal of the battery, through the resistor, to the negative plate of the capacitor.
  3. Plate Charging:
    • The positive terminal pulls electrons from one plate, leaving it positively charged.
    • The negative terminal pushes electrons onto the other plate, making it negatively charged.
  4. Insulator Role:
    • The insulator between the plates prevents charge flow, forcing charge to accumulate.
  5. Electrostatic Repulsion:
    • As negative charge builds, it repels incoming electrons, slowing the flow of charge.
  6. Current and Voltage:
    • Current decreases exponentially over time.
    • Potential difference (V) across the plates increases as charge accumulates, eventually matching the supply voltage.
  7. Fully Charged:
    • The capacitor stops charging when it reaches maximum charge, determined by its capacitance (C) and the supply voltage.
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5
Q

Discharging Capacitors

A
  1. Initial Setup:
    • A circuit with a resistor (R), switch, and capacitor (C) in series. No power supply is present.
  2. Switch Closed:
    • The potential difference (V) across the capacitor causes a current (I) to flow through the circuit.
  3. Current Flow:
    • Electrons flow from the negative plate of the capacitor, through the resistor, to the positive plate, reducing charge on both plates.
  4. Exponential Decay:
    • Current, potential difference, and charge decrease exponentially over time.
    • The rate of decrease is proportional to the amount remaining.
  5. Discharge Completion:
    • The capacitor is fully discharged when potential difference (V) and current (I) fall to zero.
  6. Energy Dissipation:
    • The electrical energy stored in the capacitor is transferred to thermal energy in the resistor.
  7. Graphs:
    • Current, potential difference, and charge follow an identical exponential decay pattern over time.
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6
Q

Energy Stored by a Capacitor

A

Charge and Potential Difference:

  • Charge (Q) is directly proportional to the potential difference (V), forming a straight-line graph.

===

Energy Stored:

  • The electrical energy stored in the capacitor is represented by the area under the potential-charge graph, forming a triangle.
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7
Q

Capacitors in Series

A
  1. Charge and Potential Difference:
    • The potential difference (p.d.) is shared between capacitors, but each stores the same charge (Q).
    • A negative charge on the left plate of C₁ induces an equal positive charge on its right plate.
    • This causes a negative charge on the left plate of C₂, equal to the positive charge on its right plate.
  2. Total Potential Difference:
    • Vtotal = V1 + V2
    • Substituting V = Q/C
      Vtotal = (Q/C1) + (Q/C2)
  3. Total Capacitance:
    • Since current (and charge Q) is the same in series, Q cancels out:
      1/Ctotal = (1/C1) + (1/C2)
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8
Q

Capacitors in Parallel

A
  1. Potential Difference:
    • All capacitors have the same potential difference (p.d.) across them.
  2. Charge Distribution:
    • The current splits across each junction, so the charge stored on each capacitor is different.
    • The total charge (Q) is the sum of the charges on each capacitor:
      Q = Q1 + Q2.
  3. Charge on Each Capacitor:
    Q1 = C1V and Q2 = C2 V, where V is the common p.d.
    • Therefore, Qtotal = (C1 + C2) V
  4. Total Capacitance:
    • Ctotal = C1 + C2 + C3 + ….
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9
Q

Time Constant

A

Time to Half (t1/2):

  • The time it takes for the charge, current, or voltage of a discharging capacitor to decrease to half its initial value.
  • Equation: t1/2 = ln(2) τ

===

Time Constant (τ):

  • Measures how long it takes for the charge, current, or voltage of a discharging capacitor to decrease to 37% of its original value, or for a charging capacitor to rise to 63% of its maximum value.
  • Equation: τ = RC where:
    • R = resistance (Ω).
    • C = capacitance (F).
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10
Q

How to verify if potential difference (V) or charge (Q) on a capacitor decreases exponentially?

A

Constant ratio method:

  • Plot a V-T graph and check if the time constant is constant,
  • when t = τ the potential difference on the capacitor will have decreased to approximately 37% of its original value

===

Logarithmic graph method

  • Plot a graph of ln(V )against time (t) and check if a straight-line graph is obtained.
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11
Q

Charging and Discharging graphs

A

Charging Graphs:

  1. p.d. and Charge vs. Time:
    • Both graphs have identical shapes, starting at 0 and increasing to a maximum value.
  2. Current vs. Time:
    • An exponential decay curve, starting at 0 and decreasing exponentially.

===

Discharge Graphs:

  1. Current, p.d., and Charge vs. Time:
    • All graphs show exponential decay curves with decreasing gradients.
    • Initial values (I₀, V₀, Q₀) start on the y-axis and decrease exponentially.
  2. Rate of Discharge:
    • High resistance: Slower discharge, current decreases, capacitor discharges slowly.
    • Low resistance: Faster discharge, current increases, capacitor discharges quickly.
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12
Q

Electric field

A

A region where a unit charge experiences an electrostatic force.

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13
Q

Electric Field Lines In a uniform electric field

A

Uniform Electric Field:

  • Field lines are equally spaced at all points.
  • Electric field strength is constant at all points.
  • The force on a test charge has the same magnitude and direction everywhere.

===

Electric Field Between Parallel Plates:

  • When a potential difference is applied, the plates become charged.
  • The electric field between the plates is uniform.
  • The field beyond the edges is non-uniform.
  • Field lines are directed from the positive to the negative plate.
  • A uniform electric field has equally spaced field lines.
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14
Q

Electric Field Lines In a radial electric field:

A

Radial Electric Field:

  • Field lines are equally spaced near the charge but spread out with distance.
  • Electric field strength and force on a test charge decrease with distance from the charge.

===

Around a Point Charge:

  • The field is radial, with lines:
    • Radially inwards for negative charges.
    • Radially outwards for positive charges.

===

Field Strength:

  • The field is stronger where lines are closer together and weaker where lines are further apart.
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15
Q

Electric Field Strength

A
  • Electrostatic force per unit positive charge
  • acting on a charge at a specific point
  • or on a stationary point charge

===

  • Describes how strong or weak an electric field is
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16
Q

Coulomb’s Law

A

Electric Fields and Coulomb’s Law:

  • All charged particles produce an electric field, exerting a force on other charges within range.

===

Coulomb’s Law:

  • The force between two charges is:
    • Proportional to the product of their charges (Qq).
    • Inversely proportional to the square of their separation (r2).

===

Charge Interactions:

  • Like charges (Qq > 0) Repulsion.
  • Opposite charges (Qq < 0) Attraction.
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17
Q

Electric Field strength of a Point Charge

A

Radial Field

  • Charged sphere acts as a point charge
  • Follows an inverse square law (1/r²)

===

Direction

  • Towards a negative charge
  • Away from a positive charge.
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18
Q

Electric Field Strength in a Uniform Field

A

Electric Field Strength in a Uniform Field:

  • Equation: E = V/d
    where:
    • E = electric field strength.
    • V = potential difference.
    • d = distance between plates.

===

Key Points:

  • Greater voltage (V): Results in a stronger field (E).
  • Greater separation (d): Results in a weaker field (E).
  • Does not apply to a radial field around a point charge.
  • Field direction: From the positive to the negative plate.

===

Derivation:

  1. Work done on a charge ( Q ):
    W = ΔV × Q
  2. Work done as force × distance:
    W = F × d
  3. Equating the two:
    F × d = ΔV × Q.
  4. Rearranging:
    F/Q = ΔV/d.
  5. Since E = F/Q
    E = ΔV/d.
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19
Q

Relative permittivity

A

Permittivity:

  • Measures how easy it is to generate an electric field in a material.

===

Relative permittivity (εr) (dielectric constant)

  • ratio of permittivity of a material to permittivity of free space (ε0):
  • εr = ε/ε0.
  • Dimensionless because it’s a ratio of two quantities with the same unit.
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20
Q

Effect of Dielectric on Capacitance

A

Dielectric in a Capacitor:

  1. Polar Molecules:
    • Align with the applied electric field, creating an opposing electric field.
    • This reduces the overall electric field, lowering the potential difference between the plates.
  2. Permittivity:
    • Reflects how well polar molecules align with the field; higher alignment = higher permittivity.
  3. Parallel Plate Capacitor:
    • Plates of area A, separated by distance d, with a dielectric of permittivity ε between them.
    • The reduction in potential difference increases the capacitance of the plates.
21
Q

Motion of Charged Particles in an Electric Field

A

Charged Particles in an Electric Field:

  1. Force and Motion:
    • Charged particles experience a force, causing them to move.
    • In a uniform electric field, particles move parallel to the field lines (direction depends on charge).
  2. Perpendicular Motion:
    • A particle moving perpendicular to the field follows a parabolic trajectory due to the constant force.
  3. Deflection:
    • Positive charges: Deflect towards the negative plate.
    • Negative charges: Deflect towards the positive plate.
    • Deflection depends on mass, charge, and speed:
      • Heavier particles deflect less.
      • Larger charges and slower particles deflect more.

===

Formulas:

  • Force: F = EQ
  • Work Done: W = Fd
  • Kinetic Energy: The force increases the particle’s kinetic energy, causing constant acceleration (Newton’s second law).
  • Perpendicular Velocity: If the particle’s velocity has a component perpendicular to the field, it remains unchanged (Newton’s first law).
22
Q

Electric Potential

A

Electric Potential:

  • Defined as the work done per unit positive charge to bring a test charge from infinity to a defined point.
  • A scalar quantity (no direction) but can be positive, negative, or zero:
    • Positive around an isolated positive charge.
    • Negative around an isolated negative charge.
    • Zero at infinity.

===

Total Electric Potential:

  • The total potential at a point from multiple charges is the sum of the potentials from each individual charge.
23
Q

The graph of potential V against distance r for a negative or positive charge

A

Electric Potential for a Positive Charge:

  • As distance (r) decreases, electric potential (V) increases.
  • More work is required to overcome the repulsive force as the test charge moves closer.
  • V starts positive and increases as r decreases, approaching zero as r approaches infinity.

===

Electric Potential for a Negative Charge:

  • As distance (r) decreases, electric potential (V) decreases (becomes more negative).
  • Less work is required due to the attractive force, which pulls the test charge closer.
  • V starts negative and decreases (in magnitude) as r decreases, approaching zero as r increases towards infinity.
24
Q

Electric Potential Energy

A

Work in an Uniform Electric Field:

  • Work is done when a charge moves through an electric field.
    • Positive charge: Work is done when it moves against the field.
    • Negative charge: Work is done when it moves with the field.

Key Points

  • The work done equals the change in electric potential energy.
  • When the electric potential is zero, the electric potential energy is also zero.
  • The work done depends on the distance the charge moves in the field.
  • q = charge being moved; Q = charge producing the potential. Do not confuse the two in calculations.

===

Work in a Radial Field:

  • Work is required to:
    • Move a positive charge closer to another positive charge (overcoming repulsion).
    • Move a positive charge away from a negative charge (overcoming attraction).

Key points

  • Potential energy increases when moving a charge towards a repelling charge and decreases when moving away from an attracting charge.
25
Q

Force-Distance Graph for a Point Charge

A

Force-Distance Graph:

  • Force (F) values are all positive.
  • As r increases, F follows a 1/r² relation (inverse square law).
  • The area under the graph represents work done (ΔW).
  • The graph shows a steep decline as r increases.

===

Estimating Area:

  • Use methods like counting squares or summing areas of trapeziums.
26
Q

Electric field between two point charges

A

Opposite Charges:

  • Field lines are directed from the positive charge to the negative charge.
  • As the charges get closer, the attractive force becomes stronger.

===

Same Type Charges:

  • Field lines are directed away from two positive charges or towards two negative charges.
  • As the charges get closer, the repulsive force becomes stronger.
  • A neutral point exists at the midpoint where the resultant electric force is zero.
27
Q

Capacitance of an Isolated Sphere

A

Capacitance of a Charged Sphere:

  • Defined as the charge per unit potential at the surface:
    C = Q / V

===

Key Equations:

  1. Potential of an Isolated Point Charge:
    V = Q / (4πε₀R)
  2. Capacitance of an Isolated Sphere:
    C = 4πε₀R

===

Variables:

  • Q = charge on the sphere (considered as a point charge at its center).
  • R = radius of the sphere.
  • ε₀ = permittivity of free space.
28
Q

Electric Fields vs Gravitational Fields

A

Similarities Between Gravitational and Electrostatic Forces:

  1. Both follow the inverse square law.
  2. Field lines around a point mass and a negative point charge are identical.
  3. Field lines in uniform gravitational and electric fields are identical.
  4. Field strengths in a radial field have a 1/r relationship.
  5. Potential in both fields has a 1/r relationship.
  6. Equipotential surfaces are:
    • Spherical around a point mass or charge.
    • Parallel in uniform fields.
  7. Work done is the product of:
    • Mass and change in gravitational potential.
    • Charge and change in electric potential.

===

Differences:

  1. Gravitational force acts on mass; electrostatic force acts on charge.
  2. Gravitational force is always attractive; electrostatic force can be attractive or repulsive.
  3. Gravitational potential is always negative; electric potential can be negative or positive.
29
Q

Magnetic Fields

A

Magnetic Field:

  • A field of force created by moving electric charges or permanent magnets, also called a B-field.

===

Sources of Magnetic Fields:

  • Permanent magnets produce magnetic fields.
  • Current-carrying wires create magnetic fields due to the movement of electrons (stationary charges do not produce magnetic fields).

===

Observing Magnetic Fields:

  • Although invisible, their effects can be observed through:
    • The force acting on magnetic materials (e.g., iron).
    • The movement of a needle in a plotting compass.
30
Q

Field Lines in a Current-Carrying Wire

A

Magnetic Field Around a Current-Carrying Wire:

  • Field lines are circular rings centered on the wire.
  • The field is strongest near the wire and weakens with distance.
  • Reversing the current reverses the direction of the field lines.

===

Maxwell’s Right-Hand Screw Rule:

  • Point your thumb in the direction of the conventional current (positive to negative).
  • The curled fingers indicate the direction of the magnetic field around the wire.
31
Q

Magnetic Field Lines in Solenoids and Coils

A

Field Lines in a Solenoid:

  • Electromagnets use solenoids (coils of wire) to concentrate magnetic fields.
  • One end becomes the north pole, and the other becomes the south pole.
  • Magnetic field lines resemble those of a bar magnet:
    • Emerge from the north pole.
    • Return to the south pole.

===

Field Lines in a Flat Circular Coil:

  • Behaves like a single loop of a solenoid.
  • Field lines:
    • Emerge from one side (north pole).
    • Return to the other side (south pole).
  • Multiple coils in a solenoid combine to create a stronger, uniform field.

===

Right-hand thumb rule:
- Thumb shows the magnetic field direction.
- Fingers show the current direction.

32
Q

Factors Affecting the Magnetic Field Strength

A
  1. Add a Ferrous Core:
    • Use a core made from a ferrous (iron-rich) material (e.g., an iron rod).
    • When current flows, the core becomes magnetised, increasing the field strength by several hundred times.
  2. Add More Turns to the Coil:
    • Concentrates the magnetic field lines, increasing the field strength.
33
Q

Fleming’s Left-Hand Rule

A

Fleming’s Left-Hand Rule:

  • Determines the direction of magnetic force on a moving charged particle in a magnetic field:
    • First Finger: Direction of the magnetic field.
    • Second Finger: Direction of conventional current (velocity of a moving positive charge).
    • Thumb: Direction of the magnetic force.

===

Magnetic Field Direction in 3D:

  • Dots (tip of an arrow): Magnetic field coming out of the page.
  • Crosses (back of an arrow): Magnetic field going into the page.
34
Q

Magnetic Flux Density

A
  • Defined as the force acting per unit current per unit length on a current-carrying conductor placed perpendicular to the magnetic field.
  • Units: Tesla (T), where 1 T = 1 N m⁻¹ force on a conductor carrying 1 A current normal to the field.
  • Also referred to as magnetic field strength.
35
Q

Force on a Current-Carrying Conductor

A

Magnetic Force on a Current-Carrying Conductor:

  • A current-carrying conductor produces its own magnetic field.
  • An external magnetic field exerts a magnetic force on the conductor.
  • The maximum force occurs when the current is perpendicular to the magnetic flux lines.

===

Magnitude of Magnetic Force (F):

  • Proportional to:
    • Current (I).
    • Magnetic flux density (B).
    • Length of conductor in the field (L).
    • Sine of the angle (θ) between the conductor and the magnetic flux lines.
  • No force is experienced if the current is parallel to the magnetic field.
36
Q

Force on a Moving Charge

A

Magnetic Force on a Moving Charged Particle:

  • Equation: F = BQv, where:
    • F = magnetic force (N).
    • B = magnetic flux density (T).
    • Q = charge of the particle (C).
    • v = speed of the particle (m/s).
  • This is the maximum force when F, B, and v are mutually perpendicular.
  • If the particle travels parallel to the magnetic field, it does not experience a magnetic force.

===

Force at an Angle θ:

  • When the particle moves at an angle θ to the magnetic field lines:
    F = BQv sin θ
37
Q

Motion of a Charged Particle in a Magnetic Field

A

Circular Motion of a Charged Particle in a Magnetic Field:

  • A charged particle in a uniform magnetic field perpendicular to its motion travels in a circular path because:
    • The magnetic force (F) is always perpendicular to its velocity (v), causing circular motion.
    • The magnetic force always points towards the center of the circular path.

===

Centripetal Force:

  • Provides the force required for circular motion:
    mv² / r = BQv
  • Rearranging for the radius r:
    r = mv / BQ

===

Key Points:

  • Faster particles (v): Move in larger circles r ∝ v
  • Greater mass (m): Move in larger circles r ∝ m
  • Greater charge (q): Move in smaller circles r ∝ 1 / q
  • ## Stronger magnetic field (B): Move in smaller circles r ∝ 1 / B
  • Calculated using Newton’s second law:
    F = ma
38
Q

Charged Particles in a Velocity Selector

A

Velocity Selector:

  • Filters charged particles by using perpendicular electric and magnetic fields to allow only particles with a specific velocity to pass through.
  • Used in devices like mass spectrometers to create a beam of particles moving at the same speed.

===

Setup:

  • Two oppositely charged plates create an electric field (E).
  • A magnetic field (B) is applied perpendicular to the electric field.

===

Force Balance:

  • Electric force: FE = EQ (independent of velocity).
  • Magnetic force: FB = BQv (depends on velocity).
  • For a particle to pass through undeflected, the forces must balance:
    FE = FB.
  • The selected velocity is:
    v = E / B.

===

Deflection:

  • Particles with velocities different from v are deflected and removed from the beam.
39
Q

Magnetic Flux

A

Magnetic Flux (Φ):

  • Defined as the product of magnetic flux density (B) and the cross-sectional area (A) perpendicular to the magnetic field:
    Φ = B A
  • Units: Webers (Wb).

===

Key Points:

  • Maximum flux: Occurs when the magnetic field lines are perpendicular to the area.
  • Minimum flux: Occurs when the magnetic field lines are parallel to the area.
  • Represents the amount of magnetic field passing through a given area.
40
Q

Magnetic Flux Linkage

A

Magnetic Flux Linkage:

  • Commonly used for solenoids with N turns of wire.
  • Defined as the product of magnetic flux (Φ) and the number of turns (N) in the coil:
    ΦN = Φ × N = B × A × N** where:
    • B = magnetic flux density.
    • A = cross-sectional area of the coil.
    • N = number of turns in the coil.
  • Units: Weber turns (Wb turns).

===

General Equation:

-ΦN = B × A × N × cos(θ) where θ is the angle between the magnetic field lines and the normal to the coil.

41
Q

Faraday’s Law

A
  • The magnitude of the induced e.m.f. (electromotive force) is directly proportional to the rate of change of magnetic flux linkage.
  • The equation form of Faraday’s Law is:
    ε = Δ(Nɸ) / Δt
    Where:
    • ε = induced e.m.f (V)
    • Δ(Nɸ) = change in flux linkage (Wb turns)
    • Δt = time interval (s)
42
Q

Lenz’s Law

A

Lenz’s Law:

  • The induced e.m.f. produces effects that oppose the change causing it.

===

Example:

  • If a north pole approaches the coil, the induced e.m.f. creates an opposing north pole to repel the incoming magnet.

===

Right-Hand Grip Rule:

  • Curl fingers around the coil in the direction of the current.
  • The thumb points along the direction of the magnetic flux (north to south).
  • In this case, the current flows anti-clockwise, inducing a north pole to oppose the incoming magnet.
43
Q

Induced E.m.f.

A

Faraday’s Law with Lenz’s Law:

The equation that combines Faraday’s Law and Lenz’s Law is written as:
ε = - Δ(Nɸ) / Δt

  • The negative sign represents Lenz’s Law.
44
Q

EMF Inducted in a Rotating Coil

A

Induced E.M.F. in a Rotating Coil:

  • When a coil rotates in a uniform magnetic field, the magnetic flux through the coil changes, causing the induced e.m.f. to change.
  • The e.m.f. is:
    • Maximum when the coil cuts through the most magnetic field lines (normal to the coil is perpendicular to the field).
    • Zero when the coil is aligned with the field (normal to the coil is parallel to the field).

===

E.M.F. Formula:

  • ε = BANω sin(θ)
  • where θ = ωt
  • The e.m.f. varies sinusoidally and is 90° out of phase with the flux linkage.
45
Q

Alternators

A

Alternator:

  • A device that converts mechanical energy into electrical energy using a rotating coil in a magnetic field.

===

Components:

  1. Coil: A rectangular coil rotates within a uniform magnetic field, generating electricity.
  2. Slip Rings: Metal rings that rotate with the coil, maintaining continuous electrical contact.
  3. Brushes: Metal brushes press against the slip rings to transfer current to the external circuit.

===

Operation:

  • As the coil rotates, it cuts through magnetic field lines, inducing a potential difference (voltage) across the coil.
  • The induced current changes direction as the coil spins, creating an alternating current (AC).
  • The meter pointer deflects first in one direction, then the opposite, as the current reverses.
  • The induced voltage and current alternate direction continuously, producing a steady AC waveform.
46
Q

Dynamos

A

Dynamo:

  • A direct-current (D.C.) generator that uses a split-ring commutator instead of slip rings.
  • Consists of a rotating coil in a magnetic field.

===

Operation:

  • The split-ring commutator ensures the current stays in one direction.
  • The induced potential difference varies only in the positive region of the graph, never reversing direction.
  • The current is always positive (or negative), never alternating.

===

Key Process:

  • As the coil rotates, it cuts through magnetic field lines, inducing a potential difference between the coil’s ends.
  • The split-ring commutator changes the coil’s connection to the brushes every half turn, keeping the current in the same direction.
  • This change occurs when the coil is perpendicular to the magnetic field lines.
47
Q

Transformer Basics

A

Transformer:

  • Changes high alternating voltage at low current to low alternating voltage at high current, and vice versa.
  • Increases transmission efficiency by reducing heat energy loss in power lines.

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Power Loss:

  • Given by P = I²R, so reducing current reduces power loss during transmission.

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Applications:

  • Used in the National Grid for efficient power transmission.
  • Step-up transformers: Increase voltage and decrease current for long-distance transmission.
  • Step-down transformers: Reduce voltage and increase current for local use near homes and businesses.
48
Q

Transformer Components and Functioning

A

Step-Up Transformer:

  • The secondary coil has more turns than the primary coil, increasing voltage.

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Operation:

  • The primary coil is powered by an alternating current (AC), creating a changing magnetic field in the iron core.
  • The changing magnetic field induces an e.m.f. in the secondary coil.
  • The secondary voltage depends on the number of turns:
    • More turns = step-up (voltage increases).
    • Fewer turns = step-down (voltage decreases).

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Components:

  • Primary coil, secondary coil, and soft iron core.
  • The soft iron core focuses and directs the magnetic field between the coils, and is used because it can be easily magnetised and demagnetised.
49
Q

Eddy Currents

A

Transformer Efficiency:

  • Transformers are not 100% efficient, and power loss occurs due to various factors.

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Eddy Currents:

  • Looping currents in the core caused by the changing magnetic flux.
  • Effects:
    • Generate heat, leading to energy loss.
    • Create a magnetic field that opposes the inducing field, reducing field strength.

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Reducing Eddy Currents:

  • The core is laminated, with layers separated by thin insulating material to prevent current flow.