Lecture 6: 555 Timer

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Lecture 6: 555 Timer. Energy storage, Periodic Waveforms, and One of the most useful electronic devices. Examples of Physical Periodic Motion. Pendulum Bouncing ball Vibrating string (stringed instrument) Circular motion (wheel) Cantilever beam (tuning fork). Other Periodic Phenomena. - PowerPoint PPT Presentation

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April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

1

Lecture 6: 555 Timer

Energy storage,Periodic Waveforms, and

One of the most useful electronic devices

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

2

Examples of Physical Periodic Motion

• Pendulum• Bouncing ball• Vibrating string (stringed instrument)• Circular motion (wheel)• Cantilever beam (tuning fork)

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

3

Other Periodic Phenomena

• Daily cycle of solar energy

• Annual cycle of solar energy

• Daily temperature cycle• Annual temperature

cycle• Monthly bank balance

cycle• Electronic clock pulse

trains• Line voltage and current

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

4

Daily Average TemperatureAlbany-Troy-Schenectady

• Data (blue) covers 1995-2002• Note the sinusoid (pink) fit to the data

-10

0

10

20

30

40

50

60

70

80

90

1

78

15

5

23

2

30

9

38

6

46

3

54

0

61

7

69

4

77

1

84

8

92

5

10

02

10

79

11

56

12

33

13

10

13

87

14

64

15

41

16

18

16

95

17

72

18

49

19

26

20

03

20

80

21

57

22

34

23

11

23

88

24

65

25

42

26

19

26

96

27

73

28

50

Series1

Series2

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

5

Using Matlab to Produce Audio Signal from Daily Average

Temps

0 200 400 600-1

-0.8

-0.6

-0.4

-0.2

0

0.2

0.4

0.6

0.8Original data (normalized)

0 200 400 600-0.5

0

0.5Sinusoid fit to data

• Data is normalized to mimic sound• Data is filtered to find fundamental

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

6

Matlab Window

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

7

Periodic Pulse Train from a 555 Timer

• This circuit puts out a steady state train of pulses whose timing is determined by the values of R1, R2 and C1

• The formula has a small error as we will see

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

8

Using Models• Recall that you should use a model that you

understand and/or know how to properly apply

• To use it properly Check for plausibility of predicted values (ballpark

test). Are the values in a reasonable range? Check the rate of changes in the values (checking

derivative or slope of plot). Are the most basic things satisfied?

• Conservation of energy, power, current, etc.

• Developing a qualitative understanding of phenomena now will help later and with simulations.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

9

Charging a Capacitor

• Capacitor C1 is charged up by current flowing through R1

• As the capacitor charges up, its voltage increases and the current charging it decreases, resulting in the charging rate shown

VV V

R1

1k

U2

TOPEN = 0

12

C1

1uF

U1

TCLOSE = 0

1 2

0

V110V

IV V

R

V

kCAPAC ITO R CAPAC ITO R

1

1

10

1

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10msV(U2:1) V(R1:2) V(V1:+)

0V

2V

4V

6V

8V

10V

Capacitor Voltage

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

10

Charging a Capacitor

• Capacitor Current

• Capacitor Voltage

• Where the time constant

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10msI(R1) I(C1)

0A

2mA

4mA

6mA

8mA

10mA

Capacitor and Resistor Current

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10msV(U2:1) V(R1:2) V(V1:+)

0V

2V

4V

6V

8V

10V

Capacitor Voltage

I I eot

V V eo

t

1

RC R C m s1 1 1

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

11

Charging a Capacitor

• Note that the voltage rises to a little above 6V in 1ms.

Time

0s 1ms 2ms 3ms 4ms 5ms 6ms 7ms 8ms 9ms 10msV(U2:1) V(R1:2) V(V1:+)

0V

2V

4V

6V

8V

10V

Capacitor Voltage

( ) .1 6321 e

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

12

Charging a Capacitor

• There is a good description of capacitor charging and its use in 555 timer circuits at http://www.uoguelph.ca/~antoon/gadgets/555/555.html

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

13

2 Minute QuizName___________

Section___True or False?

• If C1 < C2, for a fixed charging current, it will take longer to charge C1 than C2

• If R1 < R2, for a fixed charging voltage, it will take longer to charge a given capacitor C through R1 than R2

• When a capacitor C is connected to a battery through a resistor R, the charging current will be a maximum at the moment the connection is made and decays after that.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

14

555 Timer

• At the beginning of the cycle, C1 is charged through resistors R1 and R2. The charging time constant is

• The voltage reaches (2/3)Vcc in a time

( )R R C1 2 1

0 693 1 2 1. ( )R R C

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

15

555 Timer

• When the voltage on the capacitor reaches (2/3)Vcc, a switch is closed at pin 7 and the capacitor is discharged to (1/3)Vcc, at which time the switch is opened and the cycle starts over

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

16

555 Timer

• The capacitor voltage cycles back and forth between (2/3)Vcc and (1/3)Vcc at times and

1 0 693 1 2 1 . ( )R R C 2 0 693 2 1 . ( )R C

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

17

555 Timer

• The frequency is then given by

Note the error in the figure

fR R C R R C

1

0 693 1 2 2 1

1 44

1 2 2 1. ( )

.

( )

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

18

Inside the 555

• Note the voltage divider inside the 555 made up of 3 equal 5k resistors

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

19

555 Timer

• These figures are from the lab writeup• Each pin has a name (function)• Note the divider and other components inside

NE555

2

5

3

7

6

4 81

TR

CV

Q

DIS

THR

R

VC

CG

ND

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

20

Astable and Monostable Multivibrators

• Astable puts out a continuous sequence of pulses

• Monostable puts out one pulse each time the switch is connected

5V

Ra

C

0.01

uF

LED

NE555

2

5

3

7

6

4 81

TR

CV

Q

DIS

THR

R

VC

CG

ND

Rb

5V

12

1K

0.01

uFC

R

LED

NE555

2

5

3

7

6

4 81

TR

CV

Q

DIS

THR

R

VC

CG

ND

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

21

Astable and Monostable Multivibrators

• What are they good for? Astable: clock, timing signal Monostable: a clean pulse of the

correct height and duration for digital system

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

22

Optical Transmitter Circuit

Astable is used to produce carrier pulses at a frequency we cannot hear (well above 20kHz)

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

23

Optical Receiver Circuit

• Receiver circuit for transmitter on previous slide

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

24

Clapper Circuit

• Signal is detected by microphone• Clap is amplified by 741 op-amp• Ugly clap pulse triggers monostable to

produce clean digital pulse• Counter counts clean pulses to 2 and

triggers relay through the transistor

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

25

555 Timer Applications

• 40 LED bicycle light with 20 LEDs flashing alternately at 4.7Hz

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

26

555 Timer Applications

• 555 timer is used to produce an oscillating signal whose voltage output is increased by the transformer to a dangerous level, producing sparks. DO NOT DO THIS WITHOUT SUPERVISION

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

27

Tank Circuit: A Classical Method Used to Produce an Oscillating Signal

• A Tank Circuit is a combination of a capacitor and an inductor

• Each are energy storage devices

W W LIM L 1

22 W W CVE C

1

22

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

28

Tank Circuit: How Does It Work?

• Charge capacitor to 10V. At this point, all of the energy is in the capacitor.

• Disconnect voltage source and connect capacitor to inductor.

• Charge flows as current through inductor until capacitor voltage goes to zero. Current is then maximum through the inductor and all of the energy is in the inductor.

0

V110V

U2

TCLOSE = 0

1 2U1

TOPEN = 0

1 2

C1

1uF

V

L1

10uH

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

29

Tank Circuit

• The current in the inductor then recharges the capacitor until the cycle repeats.

• The energy oscillates between the capacitor and the inductor.

• Both the voltage and the current are sinusoidal.

0

V110V

U2

TCLOSE = 0

1 2U1

TOPEN = 0

1 2

C1

1uF

V

L1

10uH

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

30

Tank Circuit Voltage and Current

Time

0s 10us 20us 30us 40us 50us 60us 70us 80us 90us 100usV(C1:1)

-10V

0V

10V

SEL>>

Voltage

I(L1)-4.0A

0A

4.0A

Current

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

31

Tank Circuit

• There is a slight decay due to finite wire resistance.

• The frequency is given by (period is about 10ms)

Time

0s 10us 20us 30us 40us 50us 60us 70us 80us 90us 100usV(C1:1)

-10V

0V

10V

SEL>>

Voltage

I(L1)-4.0A

0A

4.0A

Current

fLC

1

2

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

32

Tank Circuit•Tank circuits are the basis of most oscillators. If such a combination is combined with an op-amp, an oscillator that produces a pure tone will result.

•This combination can also be used to power an electromagnet.

•Charge a capacitor

•Connect the capacitor to an electromagnet (inductor). A sinusoidal magnetic field will result.

•The magnetic field can produce a magnetic force on magnetic materials and conductors.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

33

Tank Circuit Application

• In lab 9 we will be using the circuit from a disposable camera.

• We can also use this type of camera as a power source for an electromagnet.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

34

Disposable Camera Flash Capacitor Connected to a Small Electromagnet

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

35

Disposable Camera Flash Experiment/Project

• A piece of a paperclip is placed part way into the electromagnet.

• The camera capacitor is charged and then triggered to discharge through the electromagnet (coil).

• The large magnetic field of the coil attracts the paperclip to move inside of the coil.

• The clip passes through the coil, coasting out the other side at high speed when the current is gone.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

36

Coin Flipper and Can Crusher

• The can crusher device (not presently in operation) crushes a soda can with a magnetic field.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

37

Can Crusher and Coin Flipper

• This is an animation a student made as a graphics project a few years ago

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

38

Can Crusher and Coin Flipper

• For both the can crusher and coin flipper, the coil fed by the capacitor acts as the primary of a transformer.

• The can or the coin acts as the secondary. • A large current in the primary coil produces an

even larger current in the can or coin (larger by the ratio of the turns in the primary coil)

• The current in the coin or can is such that an electromagnet of the opposite polarity is formed (Lenz’ Law) producing two magnets in close proximity with similar poles facing one another.

• The similar poles dramatically repel one another

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

39

Magnetic Launchers

• Coilguns/Railguns

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

40

Coilguns & Railguns

• Two types of launchers are being developed for a variety of purposes.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

41

Where Will You See This Material Again?

• Electromagnetic Fields and Forces: Fields and Waves I

• 555 Timers: Many courses including Analog Electronics and Digital Electronics

• Oscillators: Analog electronics• Clocks, etc: Digital Electronics,

Computer Components and Operations, and about half of the ECSE courses.

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

42

Appendix

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

43

Using Conservation Laws to Derive Fundamental Equations

• Energy stored in capacitor plus inductor

• Total energy must be constant, thus

Energy W LI CVTO TAL 1

2

1

22 2

dW

dtL I

d I

d tC V

dV

d tTO TAL 0

1

22

1

22

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

44

Using Conservation Laws

• Simplifying

• This expression will hold if

• Noting that

dW

dtLd I

d tI C

dV

d tVTO TAL L

LC

C 0

V LdI

d tLL I C

dV

d tCC

V VC L I IC L

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

45

Using Conservation Laws

• Note that for the tank circuit The same current I flows through both

components The convention is that the current

enters the higher voltage end of each component

I

+

+

VC

VL

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

46

Using Conservation Laws

• Experimentally, it was also determined that the current-voltage relationship for a capacitor is

• Experimentally, it was also determined that the current-voltage relationship for an inductor is

I CdV

d tCC

V LdI

d tLL

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

47

Using Conservation Laws

• Applying the I-V relationship for a capacitor to the expressions we saw before for charging a capacitor through a resistor

• We see that

I I eot

V V eo

t

1 I C

dV

d tCC

I I e CdV

d tCV eC o

tC

o

t

0 1

April 19, 2023

Introduction to Engineering Electronics

K. A. Connor

48

Using Conservation Laws

• Simplifying

• Which is satisfied if

• The latter is the relationship for a resistor, so the results work.

I I e CdV

d tCV eC o

tC

o

t

1

RC IV

Roo