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Page 1: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 1/89

Page 2: AC Principles Series RLC

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Page 3: AC Principles Series RLC

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The same applies to AC circuits

Current is the same in all components V supply will be the sum of VR and VXL

The total opposition to current flow, impedance in a.c.circuits, is the sum of R and XL

Page 4: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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If I = 2A, R = 40, XL = 30 Then:

Page 5: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The supply voltage would be?

100V

Page 6: AC Principles Series RLC

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WHY?????

How can 80 + 60 = 100

It must be remembered that the voltage

drop across the resistor is in phase withcurrent and the voltage drop across the

inductor leads the current by 90°

The problem must be solved as a vector or 

phasor 

Page 7: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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 As this is a series circuit current is

common to all components and is

used as reference.

Page 8: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The voltage drop across the

resistor is in phase with the current

Page 9: AC Principles Series RLC

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The voltage on the inductor leads

by 90°

Page 10: AC Principles Series RLC

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Using the end to end method VXL

can be drawn at the end of VR

Page 11: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The supply voltage can now be

found

Page 12: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The angle between the voltage and

the current is also useful

Page 13: AC Principles Series RLC

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http://slidepdf.com/reader/full/ac-principles-series-rlc 13/89

For our circuit

Page 14: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Therefore

Page 15: AC Principles Series RLC

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Total opposition to current flow

Rather thanresistance, this isreferred to as

impedance on a.c.circuits

It is still measured inohms, but has thesymbol Z

For our circuitcalculate theimpedance

Page 16: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Using Ohm¶s law

Z =V SUPPLY

I SUPPLY 

Z =100

Z = 50

Page 17: AC Principles Series RLC

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It is possible to make another 

triangle, known as an impedance

triangle

Page 18: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Our impedance triangle is shown

as:

Page 19: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The power consumed by the circuit

can now be determined

Page 20: AC Principles Series RLC

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The inductor consumes no power 

Page 21: AC Principles Series RLC

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The inductor appears to consume 120W, but

watts cannot be used. So VA, Volts x Amps,

is used. VAR for reactive

Page 22: AC Principles Series RLC

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The circuit consumes 160W but

appears to consume 200.

Page 23: AC Principles Series RLC

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Power triangle

Page 24: AC Principles Series RLC

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This can be shown as:

Page 25: AC Principles Series RLC

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Power factor 

Power factor is the ratio between true Power and

 Apparent Power.

This is also the cosine of the angle between the

True and Apparent power 

Page 26: AC Principles Series RLC

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Page 27: AC Principles Series RLC

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Using the triangles

Using Ohm¶s law (V = IR) and the power formula

(P = VI) you can move from one triangle to the

other.

Multiple by current to move to the right

Divide by current to move to the left

Page 28: AC Principles Series RLC

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Multiply or divide a side by current

to move between triangles

Page 29: AC Principles Series RLC

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Page 30: AC Principles Series RLC

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Page 31: AC Principles Series RLC

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Resistors and Capacitors on AC

Current is the same in all components V supply will be the sum of VR and VXC

The total opposition to current flow, impedance in a.c.circuits, is the sum of R and XC

Page 32: AC Principles Series RLC

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If I = 2A, R = 40, XC = 30 Then:

Page 33: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The supply voltage would be?

100V

Page 34: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 34/89

WHY?????

How can 80 + 60 = 100

It must be remembered that the voltage

drop across the resistor is in phase withcurrent and the voltage drop across the

Capacitor lags the current by 90°

The problem must be solved as a vector or 

phasor 

Page 35: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 35/89

 As this is a series circuit current is

common to all components and is

used as reference.

Page 36: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 36/89

The voltage drop across the

resistor is in phase with the current

Page 37: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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The voltage on the capacitor lags

by 90°

Page 38: AC Principles Series RLC

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Using the end to end method VXC

can be drawn at the end of VR

Page 39: AC Principles Series RLC

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Page 40: AC Principles Series RLC

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The supply voltage can now be

found

Page 41: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 41/89

The angle between the voltage and

the current is also useful

Page 42: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 42/89

For our circuit

Page 43: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 43/89

Therefore

Page 44: AC Principles Series RLC

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Total opposition to current flow

Rather thanresistance, this isreferred to asimpedance on a.c.circuits

It is still measured inohms, but has thesymbol Z

For our circuitcalculate theimpedance

Page 45: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 45/89

Using Ohm¶s law

Z =V SUPPLY

I SUPPLY 

Z =100

Z = 50

It i ibl t k th

Page 46: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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It is possible to make another 

triangle, known as an impedance

triangle

Page 47: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 47/89

Our impedance triangle is shown

as:

Page 48: AC Principles Series RLC

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The power consumed by the circuit

can now be determined

Page 49: AC Principles Series RLC

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The inductor consumes no power 

Page 50: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 50/89

The inductor appears to consume 120W, but

watts cannot be used. So VA, Volts x Amps,

is used. VAR for reactive

Page 51: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 51/89

The circuit consumes 160W but

appears to consume 200.

Page 52: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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This can be shown as:

Page 53: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Power factor 

Power factor is the ratio between true Power and

 Apparent Power.

This is also the cosine of the angle between the

True and Apparent power 

Page 54: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Summary

All three triangles are the same shape, the difference is the size, each triangle is 2

times larger/smaller than the other. Which is the value of the current

Page 55: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 55/89

Using the triangles

Using Ohm¶s law (V = IR) and the power formula

(P = VI) you can move from one triangle to the

other.

Multiple by current to move to the right Divide by current to move to the left

Page 56: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Multiply or divide a side by current

to move between triangles

Page 57: AC Principles Series RLC

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Page 58: AC Principles Series RLC

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Page 59: AC Principles Series RLC

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Series Resistor, Inductor and

Capacitor 

Current is the same in all components

V supply will be the sum of VR,VXL and VXC

The total opposition to current flow, impedance in a.c. circuits, is the sumof R, XL and XC

Page 60: AC Principles Series RLC

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If I = 2A, R = 40, XL= 45, XC = 15 Then:

Page 61: AC Principles Series RLC

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The supply voltage would be?

Page 62: AC Principles Series RLC

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Once again we need to solve via

phasor 

It must be remembered that the voltage

drop across the resistor is in phase with

current

The voltage drop across the Inductor leads

the current by 90°

The voltage drop across the Capacitor 

lags the current by 90°

As this is a series circuit current is

Page 63: AC Principles Series RLC

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 As this is a series circuit current is

common to all components and is

used as reference.

Page 64: AC Principles Series RLC

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The voltage drop across the

resistor is in phase with the current

Page 65: AC Principles Series RLC

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The voltage across the inductor 

leads by 90°

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The voltage across the Capacitor 

lags by 90°

VXL and VXC are 180° out of phase

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VXL and VXC are 180 out of phase

with each other, and therefore one

can be subtracted from the other 

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Supply voltage is the phasor sum

of VR and (VXL ± VXC)

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Total opposition to current flow

Page 73: AC Principles Series RLC

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Using Ohm¶s law

Z =V SUPPLY

I SUPPLY 

Z =100

Z = 50

It is possible to make another

Page 74: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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It is possible to make another 

triangle, known as an impedance

triangle

O i d t i l i h

Page 75: AC Principles Series RLC

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Our impedance triangle is shown

as:

Th d b th i it

Page 76: AC Principles Series RLC

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The power consumed by the circuit

can now be determined

Th i d t d it

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The inductor and capacitor 

consumes no power 

The inductor and capacitor appear to

Page 78: AC Principles Series RLC

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The inductor and capacitor appear to

consume power but do not. So VA, Volts x

 Amps, is used. VAR for reactive

Th i it 160W b t

Page 79: AC Principles Series RLC

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The circuit consumes 160W but

appears to consume 200.

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Power triangle

Page 81: AC Principles Series RLC

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This can be shown as:

Page 82: AC Principles Series RLC

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Power factor 

Power factor is the ratio between true Power and

 Apparent Power.

This is also the cosine of the angle between the

True and Apparent power 

Page 83: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

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Summary

All three triangles are the same shape, the difference is the size, each triangle is 2times larger/smaller than the other. Which is the value of the current

Page 84: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 84/89

Using the triangles

Using Ohm¶s law (V = IR) and the power formula

(P = VI) you can move from one triangle to the

other.

Multiple by current to move to the right Divide by current to move to the left

Multiply or divide a side by current

Page 85: AC Principles Series RLC

8/2/2019 AC Principles Series RLC

http://slidepdf.com/reader/full/ac-principles-series-rlc 85/89

Multiply or divide a side by current

to move between triangles

Page 86: AC Principles Series RLC

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What if XC is greater than XL?

If XC is larger than XL

then the triangle will

simply be upside down

If using Pythagoras

theorem, a negativenumber squared equals a

positive number (some

modern calculators do not

do this, so check your calculator now)

Page 89: AC Principles Series RLC

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Using the internet

On many sites XL and XC have a j in front

of them to indicate vertical component of 

triangle.

XC is also given a negative value ± jXC

This makes Kirchhoff's laws more

accurate, ie VS it the sum of VR, VXL and

VXC.

At trade level however we say VXL - VXC