4.2: Energy, Power, and Resistance

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1

What is resistance

Opposition to flow of electric current in component

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2

Definition of resistance

The resistance of a component is the voltage across the component divided by the current flowing through the component

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3

Equation for resistance

V=IR

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4

Ohm as a unit

1 Ohm is the resistance of a component when a potential difference of 1 volt is produced per ampere of current

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5

Ohm’s Law Definition

For a metallic conductor at a constant temperature, the current in the conductor is directly proportional to the potential difference across the component

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6

Temperature and resistance

In a circuit, the current will decrease over time because the heating caused by the current causes the temperature of the wire to increase over time, which increases the resistance over time.

<p>In a circuit, the current will decrease over time because the heating caused by the current causes the temperature of the wire to increase over time, which increases the resistance over time.</p>
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7

Microscopic explanation of resistance

  • Temp wire increases

  • Positive ions inside wire have more internal frequency

  • Vibrate with a greater amplitude

  • Frequency of collisions between the charge carriers and metal ions increases

  • More energy is transferred from the electrons, which heats the wire

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8

What is an Ohmic component

Component that follows Ohm’s Law

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9

I-V Characteristics: Resistor

  • Opposes flow of current

  • P.D directly proportional to current

  • Ohmic component

  • Resistance always constant

  • Behaves same way despite polarity

<ul><li><p>Opposes flow of current</p></li><li><p>P.D directly proportional to current</p></li><li><p>Ohmic component</p></li><li><p>Resistance always constant</p></li><li><p>Behaves same way despite polarity</p></li></ul>
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10

I-V Characteristics: (Filament) Lamp

  • Emits light

  • P.D and current aren’t directly proportional

  • Doesn’t obey Ohm’s law

  • Resistance isn’t constant

  • Behaves the same way despite polarity

<ul><li><p>Emits light</p></li><li><p>P.D and current aren’t directly proportional</p></li><li><p>Doesn’t obey Ohm’s law</p></li><li><p>Resistance isn’t constant</p></li><li><p>Behaves the same way despite polarity</p></li></ul>
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11

I-V Characteristics: Diode/LED

  • Allows current to flow in one direction

  • Used in standby circuits

  • P.D and current are not directly proportional

  • Behaviour depends on polarity

  • Resistance isn’t constant

  • Doesn’t obey Ohm’s Law

<ul><li><p>Allows current to flow in one direction</p></li><li><p>Used in standby circuits</p></li><li><p>P.D and current are not directly proportional</p></li><li><p>Behaviour depends on polarity</p></li><li><p>Resistance isn’t constant</p></li><li><p>Doesn’t obey Ohm’s Law </p></li></ul>
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12

I-V Characteristics: Thermistor

  • Changes resistance depending on temperature

  • Used in thermostats

  • As the temperature increases, the resistance decreases

  • used to monitor temp in ovens and engines, and to measure temperature in electrical devices

  • NEGATIVE TEMPERATURE COEFFICIENT

<ul><li><p>Changes resistance depending on temperature</p></li><li><p>Used in thermostats</p></li><li><p>As the temperature increases, the resistance decreases</p></li><li><p>used to monitor temp in ovens and engines, and to measure temperature in electrical devices</p></li><li><p>NEGATIVE TEMPERATURE COEFFICIENT</p></li></ul>
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13

I-V Characteristics: Light Dependent Resistor (LDR)

  • Allows us to monitor light intensity of surroundings

  • Made of semiconductors

  • Used in smart phones to detect surrounding light

  • Resistance decreases as light intensity increases

<ul><li><p>Allows us to monitor light intensity of surroundings</p></li><li><p>Made of semiconductors</p></li><li><p>Used in smart phones to detect surrounding light</p></li><li><p>Resistance decreases as light intensity increases</p></li></ul>
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14

Negative Temperature Coefficient (NTC)

Property of materials that experience a decrease in electrical resistance when the temperature is raised

(Example of a component is a thermistor)

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15

Positive Temperature Coefficient (PTC)

Refers to materials that experience an increase of electrical resistance when their temperature is changed

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16

Method to determine I-V Characteristics

  1. Set up components in one of the circuits (see f/c in fact sheet pack)

  2. Add ammeter in series and voltmeter in parallel

  3. Alter resistance (w variable resistor or potentiometer) to obtain a range of voltages across and currents through the component

  4. Repeat readings several times (ensures reliable results)

    1. Plot a graph with current on y-axis and voltage on x-axis

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17

What is resistivity

A constant used to remove the proportionality between 1) length and resistance and 2) ross sectional area and resistance

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18

Equation for resistivity

R=pL/A


R= resistance (Ω)

p= resistivity (Ωm)

A= cross sectional area (m2)

L= length (m)

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19

How resistivity is defined

Resistance multiplied by cross sectional area divided by length, at a constant temperature

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20

Variation of resistivity with temperature

Conductors: Resistivity increases with an increase in temp (PTC)

Insulators and semiconductors: Resistivity decreases with increase in temp (NTC)

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21

Method for determining resistivity

  1. Measure diameter of the wire with a micrometer at multiple places along the wire and find and average

  2. Determine area of wire using A=Ď€r2

  3. Using circuit attached measure the current and P.D for various different lengths (regular intervals, measured with by a ruler)

  4. Calculate resistance for each length R=V/I

  5. Plot a resistance against length and graph and use y=mx+c analysis to determine resistivity

  6. Multiply by gradient by cross-sectional area to determine resistivity

<ol><li><p>Measure diameter of the wire with a micrometer at multiple places along the wire and find and average</p></li><li><p>Determine area of wire using A=<span>Ď€r<sup>2</sup></span></p></li><li><p><span>Using circuit attached measure the current and P.D for various different lengths (regular intervals, measured with by a ruler)</span></p></li><li><p><span>Calculate resistance for each length R=V/I</span></p></li><li><p><span>Plot a resistance against length and graph and use y=mx+c analysis to determine resistivity</span></p></li><li><p><span>Multiply by gradient by cross-sectional area to determine resistivity</span></p></li></ol>
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22

Definition of Power

Power is the rate of energy transfer

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23

Unit of Power

Watts, W

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24

Equation for Power with electrical energy tansferred

P=W/t


W= electrical energy transferred (J)

t= time (which energy is being transferred) (s)

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25

Equation for Power with Voltage

P=VI


V= potential difference (V)
I= current (A)

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26

Equation for Power with current2

P=I2R


R= resistance (Ω)

I= current (A)

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27

Equation for Power with voltage2

P=V2/R


V= potential difference (V)

R= resistance (Ω)

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28

Equation for calculating energy transferred in a given time

W=VIt


W= electrical energy transferred (J)

t= time (s)

V= P.D (V)

I= current (A)

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29

What is the Volt?

A reading that indicates energy transfers across a circuit

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30

What determined the type of energy transfers across a circuit/component?

If the voltage measures a potential difference or electromotive force

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Required definition for the volt

One volt is measured across a component when one Joule of energy is transferred per one Coulomb of charge passing through the component

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The voltmeter

  • Measures P.D

  • Always in parallel

    • Ideal: has infinite resistance, so no current passes through it

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33

Potential difference definition

The energy transferred from electrical energy to other forms per unit of charge (Volts)

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Equation for potential difference

W=VQ


W= energy transferred by charge Q (J)

V= potential difference (V)

Q= charge (C)

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35

potential difference measures

Electrical energy lost in a circuit

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Potential difference location

Across a component

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37

Energy transfer of potential difference

Electrical —> something else

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38

Electromotive force (emf) definition

Energy transferred from a source to electrical energy from some other form per unit charge (volts)

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Equation for emf

W=εQ


W= energy transferred by charge (Q)

ε= electromotive force (V)

Q= charge (C)

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40

EMF measures

Electrical energy gained in a circuit

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41

Where emf is found

The power supply

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42

Energy transfer of emf

Some other store —> electrical energy

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43

Equation of energy transfer for charged particles

eV=1/2mv2


e= elementary charge for required particle (C)

V= potential difference (V)

m= mass for required particle (kg)

v= velocity of particle (ms-1)

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44

What is an electron gun

An electrical device used to produce a narrow beam of electrons

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45

How an electron gun works

A small metallic filament is heated by an electric current. Some of this fives some electrons enough energy to escape the surface of the metal (in a process called thermionic emission)

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46

Thermionic emission

The emission of electrons through the action of heat

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47

What happens when filament of electron gun is placed om a vacuum with a high potential difference that is applied between the filament and the anode

The filament acts as a cathode and free electrons accelerate towards the anode gaining kinetic energy. If the anode has a small hole in it, then electrons in line with this hole can pass through it (creating a beam of electrons)

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48

The kilowatt-hour

  • Unit of energy

  • Utility companies measure the electrical energy you use in kWh

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49

Definition of kWh

1 kilowatt-hour is the energy transferred by a device of power rating 1kW in the time of 1 hour

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50

Calculating cost of energy

Cost (pence) = number of kWh used x cost of each kWh (pence)

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51

Distinction between P.D and emf

  • P.D is loss of electrical energy whereas emf is the gain of electrical energy

  • P.D happens across components whereas emf happens across the power source

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52

Linear Particle Acceleration (LINAC)

  • Uses series of cylindrical electrodes to accelerate subatomic particles

  • The polarity of the drift tube is altered between the +ve and -ve with precise timing so that as the protons leave the tube, polarity changes so they’re attracted to the next one

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