Circuits Definitions Flashcards

1
Q

Conductors

A

A material that allows the flow of electrical charge. Good conductors have a larger amount of free charge carriers to carry a current.

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2
Q

Conservation of charge

A

The total charge in a system cannot change

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3
Q

Conventional current

A

The flow from positive to negative terminal in a cell or battery, used to describe the current in a circuit

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4
Q

Electric current

A

the rate of flow of charge

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5
Q

electron flow

A

the opposite direction to conventional current flow. Electrons flow form negative to positive terminal in a cell or battery

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6
Q

elementary charge

A

the smallest possible charge, equal to the charge of an electron

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7
Q

insulator

A

A material that has no free charge carriers and so doesn’t allow the flow of electrical charge.

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8
Q

Kirchhoff’s First Law

A

A consequence of the conservation of charge. The total

current entering a junction must equal the total current leaving it.

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9
Q

Mean Drift Velocity

A

The average velocity of an electron passing through an
object. It is proportional to the current, and inversely proportional to the number of charge carriers and the cross-sectional area of the object

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10
Q

Quantisation of Charge

A

The idea that charge can only exist in discrete packets

of multiples of the elementary charge.

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11
Q

Semiconductors

A

A material that has the ability to change its number of charge carriers, and so its ability to conduct electricity. Light dependent resistors and thermistors are both examples.

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12
Q

Diode

A

A component that allows current through in one direction only. In the correct direction, diodes have a threshold voltage (typically 0.6 V) above which current can flow.

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13
Q

Electromotive Force

A

The energy supplied by a source per unit charge passing

through the source, measured in volts.

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14
Q

Filament Lamp

A

A bulb consisting of a metal filament, that heats up and glows to produce light. As the filament increases in temperature, its resistance increases since the metal ions vibrate more and make it harder for the charge carriers to
pass through.

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15
Q

LDR

A

A light sensitive semiconductor whose resistance

increases when light intensity decreases.

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16
Q

Ohmic conductor

A

A conductor for which the current flow is directly proportional to the potential difference across it, when under constant physical conditions.

17
Q

Ohm’s Law

A

The current and potential difference through an ohmic conductor held under constant physical conditions are directly proportional, with the constant of proportionality being resistance.

18
Q

Potential Difference

A

The difference in electrical potential between two points in a circuit. It is also the work done per coulomb to move a charge from the lower potential point to the higher potential point. It is measured in Volts.

19
Q

Power

A

The rate of energy transfer in a circuit. It can be calculated as the product of the current and the potential difference between two points. It is measured in Watts.

20
Q

Resistance

A

A measure of how difficult it is for current to flow through a material.

21
Q

Resistivity

A

A measure of how difficult it is for charge to travel through a material. It is proportional to the object’s resistance and cross-sectional area, and inversely proportional to the object’s length. It is measured in Ohm metres.

22
Q

Conservation of Energy

A

Energy cannot be created or destroyed - it can only be

transferred into different forms.

23
Q

Internal Resistance

A

The resistance to the flow of charge within a source. Internal resistance results in energy being dissipated within the source.

24
Q

Kirchhoff’s Second Law

A

A consequence of the conservation of energy. The sum

of the voltages in any closed loop must equal zero.

25
Q

Lost Volts

A

The difference between a source’s emf and the terminal voltage. It is equal to the potential difference across the source’s internal resistance.

26
Q

Potential Divider

A

A method of splitting a potential difference, by connecting two resistors in series. The total potential difference is split in the ratio of their resistances.

27
Q

Resistors in Parallel

A

The potential difference across resistors connected in
parallel is identical for each resistor. The current is split between the resistors. The total resistance is equal to the inverse of the sum of the inverses of the resistances of the resistors.

28
Q

Resistors in Series

A

The current through resistors connected in series is identical for each resistor. The potential difference is split in the ratio of their resistances. The total resistance is equal to the sum of the resistances of the resistors.

29
Q

Terminal PD

A

The potential difference across the terminals of a power source. It is equal to the source’s emf minus any voltage drop over the source’s internal resistance