Datasheet KA555ID, KA555I, KA555D, KA555 Datasheet (Fairchild Semiconductor)

Page 1
©2002 Fairchild Semiconductor Corporation
www.fairchildsemi.com
Rev. 1.0.2
Features
• High Current Drive Capability (200mA)
• Adjustable Duty Cycle
• Temperature Stability of 0.005%/°C
• Timing From Msec to Hours
Applications
• Precision Timing
• Pulse Generation
• Time Delay Generation
• Sequential Timing
Description
The KA555 is a highly stable controller capable of producing accurate timing pulses. With monos table operation, the time delay is controlled by one external resistor and one capacitor. With astable operation, the frequency and duty cycle are accurately controlled with two external resistors and one capacitor.
8-DIP
8-SOP
1
1
Internal Block Diagram
F/F
OutPut
Stage
1
7
5
2
3
4
6
8
RRR
Comp.
Comp.
Discharging Tr.
Vref
Vcc
Discharge
Threshold
Control Voltage
GND
Trigger
Output
Reset
KA555
Single Timer
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KA555
2
Absolute Maximum Ratings (T
A
= 25°°°°C)
Parameter Symbol Value Unit
Supply Voltage V
CC
16 V
Lead Temperature (Soldering 10sec) T
LEAD
300 °C
Power Dissipation P
D
600 mW
Operating Temperature Range KA555/KA555I
T
OPR
0 ~ +70 / -40 ~ +85 °C
Storage Temperature Range T
STG
- 65 ~ +150 °C
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KA555
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Electrical Characteristics
(TA = 25°C, V
CC
= 5 ~ 15V, unless otherwise specified)
Notes:
1. Supply current when output is high is typically 1mA less at V
CC
= 5V
2. Tested at V
CC
= 5.0V and V
CC
= 15V
3. This will determin e maximum v alue of R
A
+ RB for 15V operation , the max . total R = 20M, and for 5V op eratio n the ma x. total
R = 6.7M
Parameter Symbol Conditions Min. Typ. Max. Unit
Supply Voltage V
CC
-4.5-16V
Supply Current *
1
(Low Stable) I
CC
VCC = 5V, RL = -36 mA V
CC
= 15V, RL = -7.515 mA
Timing Error *
2
(Monos Table) Initial Accuracy Drift with Temperature Drift with Supply Voltage
ACCUR
t/T
t/V
CC
RA = 1K to100K C = 0.1µF
-1.0 50
0.1
3.0
0.5
%
ppm/°C
%/V
Timing Error *
2
(Astable) Initial Accuracy Drift with Temperature Drift with Supply Voltage
ACCUR
t/T
t/V
CC
RA = 1K to 100K C = 0.1µF
-
2.25 150
0.3
-% ppm/°C
%/V
Control Voltage V
CC
VCC = 15V 9.0 10.0 11.0 V V
CC
= 5V 2.6 3.33 4.0 V
Threshold Voltage V
TH
VCC = 15 V - 10.0 - V V
CC
= 5V - 3.33 - V
Threshold Current *
3
I
TH
- - 0.1 0.25 µA
Trigger Voltage
V
TR
V
CC
= 5V 1.1 1.67 2.2 V
V
CC
= 15V 4.5 5 5.6 V
Trigger Current I
TR
V
TR
= 0V 0.01 2.0 µA
Reset Voltage V
RST
- 0.4 0.7 1.0 V
Reset Current I
RST
- 0.1 0.4 mA
Low Output Voltage V
OL
VCC = 15V I
SINK
= 10mA
I
SINK
= 50mA
-0.06
0.3
0.25
0.75
V V
V
CC
= 5V
I
SINK
= 5mA
-
0.05 0.35 V
High Output Voltage V
OH
VCC = 15V I
SOURCE
= 200mA
I
SOURCE
= 100mA 12.75
12.5
13.3
-V
V
V
CC
= 5V
I
SOURCE
= 100mA 2.75 3.3
-
V
Rise Time of Output t
R
- - 100 - ns
Fall Time of Output t
F
- - 100 - ns
Discharge Leakage Current I
LKG
- - 20 100 nA
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KA555
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Application Information
Table1 below is the basic operating table of 555 timer:
When the low signal input is applied to the reset terminal, the timer output remains low regardless of the threshold voltage or the trigger voltage. Only when the high signal is applied to the reset terminal, timer's output changes according to threshold voltage and trigger voltage. When the threshold voltage exceeds 2/3 of the supply voltage while the timer output is high, the timer's internal discharge Tr. turns on, lowering the threshold voltage to below 1/3 of the supply voltage. During this time, the timer output is maintained low. Later, if a low signal is applied to the trigger voltage so that it becomes 1/3 of the supply voltage, the timer's internal discharge Tr. turns off, increasing the threshold voltage and driving the timer output again at high.
1. Monos Table Operation
Table 1. Basic Operating Table
Threshold Voltage
(V
th
)(Pin6)
Trigger Voltage
(Vtr)(Pin2)
Reset(Pin4) Output(Pin3)
Discharging Tr.
(Pin7)
Don't care Don't care Low Low ON
V
th
> 2Vcc / 3 Vth > 2Vcc / 3 High Low ON
Vcc / 3 < V
th
< 2 Vcc / 3 Vcc / 3 < Vth < 2 Vcc / 3 High - -
V
th
< Vcc / 3 Vth < Vcc / 3 High High OFF
10-510-410-310-210-110010110
2
10
-3
10
-2
10
-1
10
0
10
1
10
2
10M
ΩΩ
1M
ΩΩ
10k
ΩΩ
100k
ΩΩ
R
A
=1k
ΩΩ
Capacitance(uF)
Time Delay(s)
Figure 1. Monoatable Circuit
Figure 2. Resistance and Capacitance vs.
Time delay(td)
Figure 3. Waveform s of Monostable Operation
1
5
6
7
8
4
2
3
RESET
Vcc DISCH
THRES
CONT
GND
OUT
TRIG
+Vcc
R
A
C1
C2R
L
Trigger
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KA555
5
Figure 1 illustrates a monos table circuit. In this mode, the timer generates a fixed pulse whenever the trigger voltage falls below Vcc/3. When the trigger pulse voltage applied to the #2 pin falls below Vcc/3 while the timer output is low, the timer's internal flip-flop turns the discharging Tr. off and causes the timer output to become high by charging the external capacitor C1and setting the flip-flop output at the same time. The voltage across the external capacitor C1, V
C1
increases exponentially with the time constant t=RA*C and reaches 2Vcc/3
at td=1.1R
A
*C. Hence, capacitor C1 is charged through resistor RA. The greater the time constant RAC, the longer it takes
for the V
C1
to reach 2Vcc/3. In other words, the time constant RAC controls the output pulse width. When the applied voltage to the capacitor C1 reaches 2Vcc/3, the comparator on the trigger terminal resets the flip-flop, turning the discharging Tr. on. At this time, C1 begins to discharge and the timer output converts to low. In this way, the timer operating in monos table repeats the above process. Figure 2 shows the time constant relationship based on R
A
and C. Figure 3 shows the general waveforms during monos table operation. It must be noted that, for normal operation, the trigger pulse voltage needs to maintain a minimum of Vcc/3 before the timer output turns low. That is, alth ough the output remains unaffected even if a different trigger pulse is applied while the output is high, it may be affected and the waveform not operate properly if the trigger pulse voltage at the end of the output pulse remains at below Vcc/3. Figure 4 shows such timer output abnormality.
2. Astable Operation
Figure 4. Waveforms of Monos table Operat ion (abnormal)
100m 1 10 100 1k 10k 100k
1E-3
0.01
0.1
1
10
100
10M
ΩΩ
1M
ΩΩ
100k
ΩΩ
10k
ΩΩ
1k
ΩΩ
(RA+2RB)
Capacitance(uF)
Frequency(Hz)
Figure 5. Astable Ci rcu it
Figure 6. Capac itance and Resist ance vs. Frequency
1
5
6
7
8
4
2
3
RESET
Vcc DISCH
THRES
CONT
GND
OUT
TRIG
+Vcc
R
A
C1
C2R
L
R
B
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KA555
6
An astable timer operation is achieved by adding resistor RB to Figure 1 and configuring as shown on Figure 5. In astable operation, the trigger terminal and the threshold terminal are connected so that a self-trigger is formed, operating as a multi vibrator. When the timer output is high, its internal discharging Tr. turns off and the V
C1
increases by exponential
function with the time constant (R
A+RB
)*C.
When the V
C1
, or the threshold voltage, reaches 2Vcc/3, the comparator output on the trigger terminal becomes high, resetting the F/F and causing the timer output to become low. This in turn turns on the discharging Tr. and the C1 discharges through the discharging channel formed by R
B
and the discharging Tr. When the VC1 falls below Vcc/3, the comparator output on the trigger terminal becomes high and the timer output becomes high again. The discharging Tr. turns off and the V
C1
rises ag ain.
In the above process, the section where the timer output is high is the time it takes for the V
C1
to rise from Vcc/3 to 2Vcc/3,
and the section where the timer output is low is the time it takes for the V
C1
to drop from 2Vc c/3 to Vc c/3. Wh en time r o utpu t
is high, the equivalent circuit for charging capacitor C1 is as follows:
Since the duration of the timer output high state(t
H
) is the amount of time it takes for the VC1(t) to reach 2Vcc/3,
Figure 7. Waveforms of Astable Operation
Vcc
R
A
R
B
C1 Vc1
(0-)=Vcc/
3
C
1
dv
c1
dt
−−−−−−−−
VccV0-()
RAR
B
+
−−−−−−−−−−−−−−−−−−−
=
1()
VC10+() VCC3= 2()
VC1t() VCC1
2 3
−−e
-
t
RAR
B
+()C1
−−−−−−−−−−−−−−−−−−−−−−








=
3()
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KA555
7
The equivalent circuit for discharging capacitor C1 when timer output is low as follows:
Since the duration of the timer output low state(
t
L
) is the amount of time it takes for the VC1(t) to reach Vcc/3,
Since R
D
is normally RB >> RD although related to the size of discharging Tr.,
t
L
=0.693RBC
1
(10)
Consequently, if the timer operates in astable, the period is the same with 'T=t
H+tL
=0.693(RA+RB)C1+0.693RBC1=0.693(RA+2RB)C1' because the period is the sum of the charge time and discharge
time. And since frequency is the reciprocal of the period, the following applies.
3. Frequency divider
By adjusting the length of the timing cycle, the basic circuit of Figure 1 can be made to operate as a frequency divider. Figure
8. illustrates a divide-by-three circuit that makes use of the fact that retriggering cannot occur during the timing cycle.
VC1t()
2 3
−−V
CC
V=
CC
1
2 3
−−e
-
t
H
RAR
B
+()C1
−−−−−−−−−−−−−−−−−−−−−−








= 4()
tHC1RAR
B
+()In2 0.693 RAR
B
+()C
1
== 5()
C1
R
B
R
D
VC1(0-)=2Vcc/3
C
1
dv
C1
dt
−−−−−−−−−
1
RAR
B
+
−−−−−−−−−−−−−−V
C1
0=+ 6()
VC1t()
2 3
−−V CC
e
-
t
RAR
D
+()C1
−−−−−−−−−−−−−−−−−−−−−−
= 7()
1 3
−−V
CC
2 3
−−V CC
e
-
t
L
RARD+()C1
−−−−−−−−−−−−−−−−−−−−−−
= 8()
tLC1RBRD+()In2 0.693 RBRD+()C
1
== 9()
frequency, f
1 T
−−
1.44
RA2RB+()C
1
−−−−−−−−−−−−−−−−−−−−−−−−
== 11()
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KA555
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4. Pulse Width Modulation
The timer output waveform may be changed by modulating the control voltage applied to the timer's pin 5 and changing the reference of the timer's internal comparators. Figure 9. illustrates the pulse width modulation circuit. When the continuous trigger pulse train is applied in the monos table mode, the timer output width is modulated according to the signal applied to the control terminal. Sine wave as well as other waveforms may be applied as a signal to the control terminal. Figure 10 shows an example of pulse width modulation waveform.
5. Pulse Position Modulation
If the modulating signal is applied to the control terminal while the timer is connected for astable operation as in Figure 11, the timer becomes a pulse position modulator. In the pulse position modulator, the reference of the timer's internal comparators is modulated which in turn modulates the timer output according to the modulation signal applied to the control terminal. Figure 12 illustrates a sine wave for modulation signal and the resulting output pulse position modulation : however, any wave shape could be used.
Figure 8. Waveforms of Frequency Divide r Operation
84
7
1
2
3
5
6
CONT
GND
Vcc
DISCH
THRES
RESET
TRIG
OUT
+Vcc
Trigger
R
A
C
Output
Input
Figure 9. Circuit for Pulse Width Modulation
Figure 10. Waveforms of Pulse Width Modulation
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KA555
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6. Linear Ramp
When the pull-up resistor RA in the monos table circuit shown in Figure 1 is replaced with constant current source, the VC1 increases linearly, generating a linear ramp. Figure 13 shows the linear ramp generating circuit and Figure 14 illustrates the generated linear ramp waveform s.
In Figure 13, current source is created by PNP transistor Q1 and resistor R1, R2, and R
E
.
For example, if Vcc=15V, R
E
=20kΩ, R1=5kW, R2=10kΩ, and VBE=0.7V,
V
E
=0.7V+10V=10.7V Ic=(15-10.7)/20k=0.215mA When the trigger is started in a timer configured as shown in Figure 13, the current flowing to capacitor C1 becomes a constant current generated by PNP transistor and resistors.
84
7
1
2
3
5
6
CONT
GND
Vcc
DISCH
THRES
RESET
TRIG
OUT
+Vcc
R
A
C
R
B
Modulation
Output
Figure 11. Circuit for Pulse Position Modulation
Figure 12. Waveforms of pulse posit ion modulation
Figure 13. Circuit for Linear Ramp
Figure 14. Waveforms of Linear Ramp
1
5
6
7
8
4
2
3
RESET
Vcc DISCH
THRES
CONT
GND
OUT
TRIG
+Vcc
C2
R1
R2
C1
Q1
Output
R
E
I
C
VCCV
E
R
E
−−−−−−−−−−−−−−−−
= 12()
Here, V
E is
VEV
BE
R
2
R1R
2
+
−−−−−−−−−−−−−V
CC
+= 13()
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KA555
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Hence, the VC is a linear ramp function as shown in Figure 14. The gradient S of the linear ramp function is defined as follows:
Here the Vp-p is the peak-to-peak voltage. If the electric charge amount accumulated in the capacitor is divided by the capacitance, the V
C
comes out as follows:
V=Q/C (15)
The above equation divided on both sides by T gives us
and may be simplified into the following equation.
S=I/C (17)
In other words, the gradient of the linear ramp function appearing across the capacitor can be obtained by using the constant current flowi ng through the capacitor. If the constant current flow through the capacitor is 0.215mA and the capacitance is 0.02uF, the gradient of the ramp function at both ends of the capacitor is S=0.215m/0.022u=9.77V/ms.
S
V
pp
T
−−−−−−−−−−
= 14()
V T
−−
QT
C
−−−−−−−
= 16()
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KA555
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Mechanical Dimensions
Package
Dimensions in millimeters
6.40 ±0.20
3.30 ±0.30
0.130 ±0.012
3.40 ±0.20
0.134 ±0.008
#1
#4 #5
#8
0.252
±0.008
9.20 ±0.20
0.79
2.54
0.100
0.031
()
0.46
±0.10
0.018 ±0.004
0.060 ±0.004
1.524 ±0.10
0.362 ±0.008
9.60
0.378
MAX
5.08
0.200
0.33
0.013
7.62
0~15°
0.300
MAX
MIN
0.25
+0.10 –0.05
0.010
+0.004
–0.002
8-DIP
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KA555
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Mechanical Dimensions
(Continued)
Package
Dimensions in millimeters
4.92 ±0.20
0.194 ±0.008
0.41 ±0.10
0.016 ±0.004
1.27
0.050
5.72
0.225
1.55 ±0.20
0.061 ±0.008
0.1~0.25
0.004~0.001
6.00 ±0.30
0.236 ±0.012
3.95 ±0.20
0.156 ±0.008
0.50 ±0.20
0.020 ±0.008
5.13
0.202
MAX
#1
#4
#5
0~8°
#8
0.56
0.022
()
1.80
0.071
MAX0.10
MAX0.004
MAX
MIN
+
0.10
-0.05
0.15
+
0.004
-0.002
0.006
8-SOP
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KA555
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Ordering Information
Product Number Package Operating Temperature
KA555 8-DIP
0 ~ +70°C
KA555D 8-SOP
KA555I 8-DIP
-40 ~ +85°C
KA555ID 8-SOP
Page 14
KA555
7/16/02 0.0m 001
Stock#DSxxxxxxxx
2002 Fairchild Semiconductor Corporation
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FAIRCHILD’S PRODUCTS ARE NOT AUTHORIZED FOR USE AS CRITICAL COMPONENTS IN LIFE SUPPORT DEVICES OR SYSTEMS WITHOUT THE EXPRESS WRITTEN APPROVAL OF THE PRESIDENT OF FAIRCHILD SEMICONDUCTOR CORPORATION. As used herein :
1. Life support devices or systems are devices or systems
which, (a) are intended for surgical implant into the body, or (b) support or sustain life, and (c) whose failure to perform when properly used in accordance with instructions for use provided in the labeling, can be reasonably expected to result in a significant injury of the user.
2. A critical component in any component of a life support device or sys tem whose failure to perform can be reasonably expec ted to cause the failur e of the life support device or system, or to affect its safety or effec tiveness.
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