Electricity (2) Flashcards
(49 cards)
Capacitors
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.
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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.
Capacitance
Capacitance:
- Defined as the charge stored per unit potential difference.
- Units: Farads (F), often in smaller units like μF, nF, or pF.
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Capacitance Equation:
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C = Q / V where:
- C = capacitance.
- Q = charge stored.
- V = potential difference.
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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.
Use of capacitors
- 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.
Charging capacitor
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Initial Setup:
- A circuit with a battery (e.m.f. ε), resistor (R), capacitor (C), and switch connected in series.
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Switch Closed:
- Electrons flow from the negative terminal of the battery, through the resistor, to the negative plate of the capacitor.
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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.
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Insulator Role:
- The insulator between the plates prevents charge flow, forcing charge to accumulate.
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Electrostatic Repulsion:
- As negative charge builds, it repels incoming electrons, slowing the flow of charge.
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Current and Voltage:
- Current decreases exponentially over time.
- Potential difference (V) across the plates increases as charge accumulates, eventually matching the supply voltage.
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Fully Charged:
- The capacitor stops charging when it reaches maximum charge, determined by its capacitance (C) and the supply voltage.
Discharging Capacitors
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Initial Setup:
- A circuit with a resistor (R), switch, and capacitor (C) in series. No power supply is present.
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Switch Closed:
- The potential difference (V) across the capacitor causes a current (I) to flow through the circuit.
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Current Flow:
- Electrons flow from the negative plate of the capacitor, through the resistor, to the positive plate, reducing charge on both plates.
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Exponential Decay:
- Current, potential difference, and charge decrease exponentially over time.
- The rate of decrease is proportional to the amount remaining.
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Discharge Completion:
- The capacitor is fully discharged when potential difference (V) and current (I) fall to zero.
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Energy Dissipation:
- The electrical energy stored in the capacitor is transferred to thermal energy in the resistor.
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Graphs:
- Current, potential difference, and charge follow an identical exponential decay pattern over time.
Energy Stored by a Capacitor
Charge and Potential Difference:
- Charge (Q) is directly proportional to the potential difference (V), forming a straight-line graph.
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Energy Stored:
- The electrical energy stored in the capacitor is represented by the area under the potential-charge graph, forming a triangle.
Capacitors in Series
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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.
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Total Potential Difference:
- Vtotal = V1 + V2
- Substituting V = Q/C
Vtotal = (Q/C1) + (Q/C2)
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Total Capacitance:
- Since current (and charge Q) is the same in series, Q cancels out:
1/Ctotal = (1/C1) + (1/C2)
- Since current (and charge Q) is the same in series, Q cancels out:
Capacitors in Parallel
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Potential Difference:
- All capacitors have the same potential difference (p.d.) across them.
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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.
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Charge on Each Capacitor:
Q1 = C1V and Q2 = C2 V, where V is the common p.d.- Therefore, Qtotal = (C1 + C2) V
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Total Capacitance:
- Ctotal = C1 + C2 + C3 + ….
Time Constant
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
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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.
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Equation: τ = RC where:
- R = resistance (Ω).
- C = capacitance (F).
How to verify if potential difference (V) or charge (Q) on a capacitor decreases exponentially?
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
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Logarithmic graph method
- Plot a graph of ln(V )against time (t) and check if a straight-line graph is obtained.
Charging and Discharging graphs
Charging Graphs:
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p.d. and Charge vs. Time:
- Both graphs have identical shapes, starting at 0 and increasing to a maximum value.
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Current vs. Time:
- An exponential decay curve, starting at 0 and decreasing exponentially.
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Discharge Graphs:
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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.
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Rate of Discharge:
- High resistance: Slower discharge, current decreases, capacitor discharges slowly.
- Low resistance: Faster discharge, current increases, capacitor discharges quickly.
Electric field
A region where a unit charge experiences an electrostatic force.
Electric Field Lines In a uniform electric field
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.
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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.
Electric Field Lines In a radial electric field:
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.
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Around a Point Charge:
- The field is radial, with lines:
- Radially inwards for negative charges.
- Radially outwards for positive charges.
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Field Strength:
- The field is stronger where lines are closer together and weaker where lines are further apart.
Electric Field Strength
- Electrostatic force per unit positive charge
- acting on a charge at a specific point
- or on a stationary point charge
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- Describes how strong or weak an electric field is
Coulomb’s Law
Electric Fields and Coulomb’s Law:
- All charged particles produce an electric field, exerting a force on other charges within range.
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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).
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Charge Interactions:
- Like charges (Qq > 0) Repulsion.
- Opposite charges (Qq < 0) Attraction.
Electric Field strength of a Point Charge
Radial Field
- Charged sphere acts as a point charge
- Follows an inverse square law (1/r²)
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Direction
- Towards a negative charge
- Away from a positive charge.
Electric Field Strength in a Uniform Field
Electric Field Strength in a Uniform Field:
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Equation: E = V/d
where:- E = electric field strength.
- V = potential difference.
- d = distance between plates.
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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.
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Derivation:
- Work done on a charge ( Q ):
W = ΔV × Q - Work done as force × distance:
W = F × d - Equating the two:
F × d = ΔV × Q. - Rearranging:
F/Q = ΔV/d. - Since E = F/Q
E = ΔV/d.
Relative permittivity
Permittivity:
- Measures how easy it is to generate an electric field in a material.
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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.
Effect of Dielectric on Capacitance
Dielectric in a Capacitor:
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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.
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Permittivity:
- Reflects how well polar molecules align with the field; higher alignment = higher permittivity.
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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.
Motion of Charged Particles in an Electric Field
Charged Particles in an Electric Field:
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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).
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Perpendicular Motion:
- A particle moving perpendicular to the field follows a parabolic trajectory due to the constant force.
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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.
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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).
Electric Potential
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.
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Total Electric Potential:
- The total potential at a point from multiple charges is the sum of the potentials from each individual charge.
The graph of potential V against distance r for a negative or positive charge
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.
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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.
Electric Potential Energy
Work in an Uniform Electric Field:
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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.
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Work in a Radial Field:
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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.