Chapter 10 Alternating Currents Flashcards

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1
Q

An alternating current (a.c) is defined as

A
  • A current which periodically varies from positive to negative and changes its magnitude continuously with time
  • This means the direction of an alternating current varies every half cycle
  • The variation of current, or p.d., with time can be described as a sine curve ie. sinusoidal
  • Therefore, the electrons in a wire carrying a.c. move back and forth with simple harmonic motion
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2
Q

As with SHM, the relationship between time period T and frequency f of an alternating current is given by:

A
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3
Q

Peak current (I0), or peak voltage (V0), is defined as:

A

The maximum value of the alternating current or voltage

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4
Q

Peak current, or voltage, can be determined from the amplitude of the graph

A
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5
Q

Mains electricity is supplied as alternating current

A
  • Power stations produce alternating current
  • This is the type of current supplied when devices are plugged into sockets
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6
Q

The equation representing alternating current which gives the value of the current I at any time t is:

A
  • I = I0 sin(⍵t)
  • Where:
    • I = current (A)
    • I0 = peak current (A)
    • ⍵ = angular frequency of the supply (rad s-1)
    • t = time (s)
    • Note: this a sine function since the alternative current graph is sinusoidal
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7
Q

A similar equation can be used for representing alternating voltage:

A

V = V0 sin(⍵t)

Where:
V = voltage (V)
V0 = peak voltage (V)
Recall the relation the equation for angular frequency ⍵:

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8
Q

Root-Mean-Square Current

A
  • Root-mean-square (r.m.s) values of current, or voltage, are a useful way of comparing a.c current, or voltage, to its equivalent direct current, or voltage
  • The r.m.s values represent the d.c current, or voltage, values that will produce the same heating effect, or power dissipation, as the alternating current, or voltage
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9
Q
  • The r.m.s value of an alternating current is defined as:
A

The value of a constant current that produces the same power in a resistor as the alternating current

  • The r.m.s current Ir.m.s is defined by the equation:
  • So, r.m.s current is equal to 0.707 × I0, which is about 70% of the peak current I0
  • The r.m.s value of an alternating voltage is defined as:

The value of a constant voltage that produces the same power in a resistor as the alternating voltage

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10
Q
  • The r.m.s voltage Vr.m.s is defined by the equation:
A
  • Where:
    • I0 = peak current (A)
    • V0 = peak voltage (V)
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11
Q
  • The r.m.s value is therefore defined as:
A

The steady direct current, or voltage, that delivers the same average power in a resistor as the alternating current, or voltage

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12
Q
  • A resistive load is any electrical component with resistance eg. a lamp
A

Vr.m.s and peak voltage. The r.m.s voltage is about 70% of the peak voltage

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13
Q

Mean Power

A
  • In mains electricity, current and voltage are varying all the time
  • This also means the power varies constantly, recall the equations for power:
  • Where:
    • I = direct current (A)
    • V = direct voltage (A)
    • R = resistance (Ω)
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14
Q

The r.m.s values means equations used for direct current and voltage can now be applied to

A
  • alternating current and voltage
  • These are also used to determine an average current or voltage for alternating supplies
  • Recall the equation for peak current:

l0= √2 Ir.m.s

  • Therefore, the peak (maximum) power is related to the mean (average) power by:

Pmean= Ir.m.sR

Pmean= P/2

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15
Q

The mean power in a resistive load

A

is half the maximum power for a sinusoidal alternating current or voltage

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16
Q
  • Rectification is defined as:
A

The process of converting alternating current and voltage into direct current and voltage

17
Q

Rectification is used in electronic equipment which requires a

A

direct current

  • For example, mains voltage must be rectified from the alternating voltage produced at power stations
18
Q

There are two types of rectification

A
  • Half-wave rectification
  • Full-wave rectification
19
Q

For half-wave rectification

A
  • The graph of the output voltage Vout against time is a sine curve with the positive cycles and a flat line (Vout = 0) on the negative cycle
  • This is because the diode only conducts in the positive direction
20
Q

For full-wave rectification:

A
  • The graph of the output voltage Vout against time is a sine curve where the positive cycles and the negative cycles are both curved ‘bumps’
21
Q

The difference between the graphs of full-wave and half-wave rectification

A
22
Q

Half-wave rectification consists of a

A
  • single diode
    • An alternating input voltage is connected to a circuit with a load resistor and diode in series
  • The diode will only conduct during the positive cycles of the input alternating voltage,
    • Hence there is only current in the load resistor during these positive cycles
  • The output voltage Vout across the resistor will fluctuate against against time in the same way as the input alternating voltage except there are no negative cycles
  • This type of rectification means half of the time the voltage is zero
  • So, the power available from a half-wave rectified supply is reduced
23
Q

Full-wave rectification requires a

A
  • bridge rectifier circuit
    • This consists of four diodes connected across an input alternating voltage supply
  • The output voltage Vout is taken across a load resistor
  • During the positive cycles of the input voltage, one terminal if the voltage supply is positive and the other negative
    • Two diodes opposite each other that are in forward bias will conduct
    • The other two in reverse bias will not conduct
    • A current will flow in the load resistor with the positive terminal at the top of the resistor
  • During the negative cycles of the input voltage, the positive and negative terminals of the input alternating voltage supply will swap
    • The two diodes that were forward bias will now be in reverse bias and not conduct
    • The other two in reverse bias will now be in forward bias and will conduct
    • The current in the load resistor will still flow in the same direction as before
24
Q

In full-wave both the positive and negative cycles s, the current in the load resistor is the…

A
  • same
  • Each diode pair is the same as in half-wave rectification
    • Since there are two pairs, this equates to full-wave rectification overall
  • The main advantage of full-wave rectification compared to half-wave rectification is that there is more power available
    • Therefore, a greater power is supplied on every half cycle
25
Q

When A is positive and B is negative, diodes 2 and 3 will conduct and 1 and 4 will not. When A is negative and B is positive, diodes 1 and 4 will conduct and diodes 2 and 3 will not. The current in the load resistor R will flow downwards

A
26
Q

Smoothing

A
  • In rectification, to produce a steady direct current or voltage from an alternating current or voltage, a smoothing capacitor is necessary
  • Smoothing is defined as:

The reduction in the variation of the output voltage or current

27
Q

Smoothing works in the following ways:

A
  • A single capacitor with capacitance C is connected in parallel with a load resistor of resistance R
  • The capacitor charges up from the input voltage and maintains the voltage at a high level
  • As it discharges gradually through the resistor when the rectified voltage drops but the voltage then rises again and the capacitor charges up again
  • The resulting graph of a smoothed output voltage Vout and output current against time is a ‘ripple’ shape
28
Q

A smoothing capacitor connected in parallel with the load resistor. The capacitor charges as the output voltage increases and discharges as it decreases

A
29
Q

A smooth, rectified current graph creates a ‘rippling’ shape against time

A
30
Q

The amount of smoothing is controlled by the

A
  • capacitance C of the capacitor and the resistance R of the load resistor
    • The less the rippling effect, the smoother the rectified current and voltage output
  • The slower the capacitor discharges, the more the smoothing that occurs ie. smaller ripples
  • This can be achieved by using:
    • A capacitor with greater capacitance C
    • A resistance with larger resistor R
  • Recall that the product RC is the time constant τ of a resistor
  • This means that the time constant of the capacitor must be greater than the time interval between the adjacent peaks of the output signal