B.5 Current and circuits Flashcards

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1
Q

Electrical Conductors

A

Materials that allow electricity to flow easily due to the movement of electrons. Metals are common examples

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2
Q

Electrical Insulators

A

Materials that do not allow electricity to flow easily. Examples include wood and rubber, which have fewer mobile charge carriers

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3
Q

Electric Potential Difference (Voltage)

A

The work done per unit charge in moving a positive charge between two points. It is measured in volts (V).

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4
Q

Electric Current

A

The rate of flow of charge, measured in amperes (A). Represents how much charge flows past a point per second

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5
Q

Electromotive Force (emf)

A

The energy that a source of electrical energy transfers to each unit of charge. Measured in volts (V)

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6
Q

Ohm’s Law

A

States that the current through a conductor between two points is directly proportional to the voltage across the two points. Represented as V = IR

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7
Q

Resistance (R)

A

A measure of the difficulty encountered by current when flowing through a conductor. Calculated as R=V/I, measured in ohms (Ω)

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8
Q

Resistivity (ρ)

A

A material’s intrinsic property indicating how strongly it resists current flow. Calculated as ρ=RA/L, measured in ohm meters (Ω⋅m)

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9
Q

Ohmic vs. Non-Ohmic Conductors

A

Ohmic conductors have a constant resistance over a range of voltages, showing a linear V-I relationship. Non-ohmic conductors display a non-linear V-I relationship, with resistance varying with voltage

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10
Q

Factors Affecting Resistance

A

The resistance of a conductor depends on its material (resistivity), length, and cross-sectional area. Longer wires and thinner wires have higher resistance

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11
Q

Series Circuit

A

A circuit where components are connected in a single path. The current is the same through all components, but the voltage divides among them

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12
Q

Parallel Circuit

A

A circuit where components are connected across common points or junctions, offering multiple paths for the current. Voltage is the same across each component

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13
Q

Current in Series

A

In a series circuit, the current is the same through all components because there is only one path for electron flow

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14
Q

Current in Parallel

A

In a parallel circuit, the total current is the sum of the currents through each parallel branch

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15
Q

Voltage in Series and Parallel

A

In series circuits, voltages add up to the source voltage. In parallel circuits, all components share the same voltage

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16
Q

Electromotive Force (emf)

A

The maximum potential difference between two electrodes of a cell; measures the energy provided per coulomb of charge.

17
Q

Internal Resistance (r)

A

The resistance within the battery or cell itself, which causes a decrease in the output voltage when a current flows.

18
Q

Total Voltage Equation for a Cell

A

Given by ϵ=I(R+r), where ϵ is the emf,
I the current, R the external resistance, and r the internal resistance

19
Q

Terminal Voltage (V)

A

The voltage measured across the terminals of a battery or cell, calculated as ϵ−Ir, where I is the current and r is the internal resistance

20
Q

Variable Resistors

A

Components that allow the resistance within a circuit to be adjusted. Used to control current flow without changing the circuit layout

21
Q

Power in Electrical Circuits

A

The rate at which electrical energy is transferred by an electric circuit. It is calculated as Power (P) = Voltage (V) × Current (I), measured in watts (W)

22
Q

The Law of Conservation of Energy in Circuits

A

States that energy cannot be created or destroyed in an isolated system. In electrical circuits, the total energy supplied by the source equals the energy converted into other forms

23
Q

Kirchhoff’s Voltage Law

A

In any closed loop in a circuit, the sum of all the voltages around the loop is equal to zero. This is due to the conservation of energy

24
Q

Kirchhoff’s Current Law

A

The total current entering a junction equals the total current leaving the junction. This law is based on the principle of conservation of charge

25
Q

The Principle of Superposition in Circuits

A

In a linear network with several independent sources, the voltage and current in any part of the network can be found by adding the voltages and currents from each source separately