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Electronics Projects chosen for approval by P. MUZHUMADHI
B. Tech – ICE Dept
Advanced LED temperature indicator Project Option I
APPLICATION OF THIS PROJECT
This project illustrates the use of a V/F converter in monitoring temperature in degrees Fahrenheit (0F). The
block diagram of the temperature indicator is shown in Figure 1-1. The indicator is composed of a
temperature sensor, amplifier, V/F converter, three-digit binary-coded-decimal (BCD) counter, time base, and
LED display In addition to the 9400 V/F converter, other ICs needed for this project include the LM334
temperature sensor, LF353 dual op-amp, NE555 timers, 74LS00 NAND gate, MC14553 three-digit BCD
counter. MC14543 BCD-to-seven segment decoder/driver/latch and three seven-segment (common anode or
common cathode) LED displays with three PNP switching transistors.
Working of the system
Figure 1-2 shows the schematic diagram, which is designed to display temperatures from 0° to
100°F. Operation of the circuit is as follows. The output of the temperature sensor changes linearly
as a function of temperature (10 mV/ K). This output is an input to the summing amplifier, which is
used to calibrate the output of the temperature sensor for a desired temperature type (K, 0C, or 0F)
and an intended range. That is, to display the temperature in either K, °C, or 0F, potentiometer R4 is
adjusted accordingly so that a suitable voltage appears at the output of the summing amplifier. Since
the output of the temperature sensor is directly proportional to temperature changes-, R4 needs to be
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adjusted at only one temperature. The output of the summing amplifier then drives the inverting amplifier. The purpose of the inverting amplifier is twofold: (1) to invert the input so that its output voltage is positive,
which is necessary for the V/F converter, and (2) to provide a suitable gain, which depends on the voltage-to-frequency
scaling used for the V/F converter.
The output of the inverting amplifier is the input to the V/F converter; therefore, the output frequency of the converter is
directly proportional the output voltage of the inverting amplifier. For example, as the temperature goes up the output
voltage of the summing amplifier increases in the negative direction, Whereas that of the inverting amplifier increases in
the positive direction, which in turn causes the frequency of the V/F to increase in the positive direction.
The output frequency of the converter is then ANDed with the gating signal to produce the clock signal for the three-digit
BCD counter. The BCD output of the counter drives the three LED displays sequentially via the BCD-to-seven segment
decoder/latch/driver stage, and the temperature is displayed on the LEDs, depending on the relationship between the
frequency of the V/F converter and the gate signal. The gate, latch, and reset signals are generated by the time-base
circuit, which consists of a free-running multivibrator and two one-shot multivibrators.
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PARTS LISTS Resistors (all ¼-watt, ± 5% Carbon)
R1 = 1 kΩ potentiometer at 230 Ω
R2, R7, R12, R13, R21 = 10 kΩ
R3, R5, R6, R11 = 100 kΩ
R4 = 10 kΩ potentiometer
R8= 1 MΩ potentiometer
R9 = 180 kΩ
R10, R15 = 50 kΩ potentiometer
R14 = 510 kΩ
R16 = 3 kΩ potentiometer
R17 = 15 kΩ
R18 = 20 kΩ
R19 = 10 kΩ potentiometer
R20 = 1 kΩ potentiometer
R22 – R28 = 220 Ω
R29 – R31 = 1k Ω
Capacitors
C1 = 1000 pF
C2 = 100 pF
C3, C6, C9 = 1 µF
C4, C5, C7, C8, C10 = 0.01 µF
C11 = 0.001 µF
Semiconductors
IC1 = LM334 temperature sensor
IC2 = LF353 dual op-amp
IC3 = Teledyne 9400 V/F convertor
IC4 = 74LS00 NAND gate
IC5, IC6, IC7 = NE/SE 555 timers
IC8 = MC 14553 three-digit BCD counter
IC9 = MC 14543 BCD-to-seven segment decoder/driver/latch
Q1, Q2, Q3 = 2N1305 switching transistors
D1, D2 = 1N914 signal diodes
Three seven-segment common anode LEDs: MAN72A or equivalent
Circuit Description
Next let us examine the design considerations and procedures for each of the sections in the
temperature indicator of Figure l-2. The temperature sensor LM334 is a three-terminal adjustable
current source whose current can be programmed from 1µ to 10 mA with one external resistor R1.
The three terminals are labeled +V, R, and –V. The pin diagram of the LM334 is shown separately in
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Figure 1-3.
The LM334 has a wide operating voltage range of 1 to 40 V. It can also withstand reverse voltage of
up to 20 V(terminal + V is negative with respect to –V). It is designed to operate over a temperature
range of 0° to 70°C. For a wider temperature range, such as -550 to 150°C, Intersil’s AD590
temperature sensor is recommended.
For the values indicated in Figure 1-2, the output of the LM334 changes 10 mV/K. This means that
at 00F = 255.22 K the output of the sensor will be 2552.2 mV, which must be scaled down to 0 V so
that the temperature displayed will be in degrees Fahrenheit. This is accomplished by the use of the
summing amplifier. Specifically, potentiometer R4 of the summing amplifier is adjusted so that the
output is 0 V. The same procedure is used to calibrate the output of the summing amplifier at any
other value of 0F. Table 1-1 shows the relationship between K, °C, 0F, and the output of the
temperature sensor and the summing amplifier at corresponding values of temperature. Because the
output of the sensor directly proportional to the temperature, the output of the summing amplifier
needs to be calibrated at the temperature at which the circuit is initially started up (refer to Table 1-
1).
Table 1-1
RELATIONSHIP BETWEEN DIFFERENT TEMPERATURE UNITS AND OUTPUTS OF THE SENSOR
AND SUMMING AMPLIFIER
Kelvin (K) Degrees Celsius Degrees Fahrenheit Output of the
temperature sensor
(mV)
Output of the
summing amplifier
(mV) to be adjusted
to
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255.22 -17.78 0 2552.2 0
273 0 32 2730 -177.8
298 25 77 2980 -427.8
310.78 37.78 100 3107.8 -555.6
Note that the output of the summing amplifier is a negative dc voltage since the net input voltage is
always positive for temperatures >00 (see Table 1-1). However, the 9400 V/F requires a positive
input voltage. The summing amplifier must be therefore be followed by an inverting amplifier. The
gain of the inverting amplifier, however, depends on the voltage-to-frequency scaling of the
convertor. The V/F convertor of figure 1-2 is calibrated for the maximum frequency of 50 KHz,
which represents a temperature of 1000F when the input voltage is 10 V maximum. Since the output
of the summing amplifier is -555.6 mV at 1000F, the gain of the inverting amplifier must be equal to
10V/555.6mV = 17.9985
The output frequency of the V/F converter is then ANDed with the output frequency (called the gate
signal) of the 555 free-running multivibrator to produce the clock signal for the three-digit BCD
counter. Since the maximum 50-kHz output frequency of the converter represents 1000F, the three-
digit BCD counter must be clocked 100 times to display I00°F. To accomplish this, the pulse width of
the free-running multivibrator must be 100/50 K = 2 ms so that 100 pulses will be produced in 2
ms. At the end of 2 ms, the count of the counter is latched and displayed on the LED display. After
the count is displayed as a temperature on the LEDs, the BCD counter is reset and the cycle repeats.
In other words, the counter continuously cycles through three states: count, latch, and reset.
Therefore, the free-running multivibrator (gate signal) must provide for the time period required to
count, latch, and reset the BCD counter. The latch enable and master reset pulses for the BCD
counter MCl4553 are produced by using two 555 one-shot multivibrators. Where the time period of
the free-running multivibrator is approximately 12.5 ms with a pulse width of 2 ms. The pulse width
of the latch enable pulse is approximately 10 ms, and the master reset pulse width is approximately
0.5 ms. To accomplish 2-, 10-, and 0.5-ms pulse widths, adjust potentiometers R16, R18, and R20,
respectively (Figure l-2).
The three-digit BCD counter used in Figure 1-2 is the MC14553. The MCl4553 consists of three
negative-edge-triggered BCD counters with a quad latch at the output of each counter, which
enables the storage of any given count. The outputs of the latches are time multiplexed so that one
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BCD digit at a time is produced. The operation of the multiplexer output selector is controlled by the
on-chip oscillator, whose frequency depends on the external capacitor.
As shown in Figure 1-2, the master reset (MR) and latch enable (LE) pulses for the MC14553 are
produced by using two 555 one-shot multivibrators. In addition, the clock signal for the MC14553 is
produced by ANDing the output of the V/F converter with the gating signal, which is obtained by
using the 555 free-running multivibrators. The digit select outputs DS1, DS2, and DS3 sequentially
drive the 2N1305 PNP transistors T1, T2, and T3, which in turn control the three LED displays. The
BCD outputs of the MCl4553 are connected to the BCD inputs of the MCl4543, which is a BCD-to-
seven segment latch/decoder/driver. The seven-segment outputs of the MCl4543 then drive the
seven segments of the LED selected by the digit-select of the MC14553.
The MCl4543 is designed to provide three functions: a 4-bit storage latch, an 8421 BCD-to-seven
segment decoder, and a driver. The device is capable of driving LCD and LED displays.
The PH pin 6 of the MC14543 is connected to VDD (logic 1) because the LED displays are the
common anode type. To limit the current through each of the LED segments, a separate resistor is
used in series with each segment. Note, however, that only seven resistor are required for all the
segment of LEDs. This is possible because the digit-select output of the MC14553 function
sequentially. In addition, the BCD output are also multiplexed, one BCD digit at a time.
Finally, since the accuracy of the temperature displayed depends mainly on the frequency stability of
the free-running multivibrator, all resistors must be of 5% or better tolerance, and capacitor must be
either Mylar of tantalum types. Also remember that the temperature indicator must be calibrated at
a temperature at which it is initially turned on.
Digital Mains Failure/Resumption Alarm Project Option II
APPLICATION OF THIS PROJECT
AC mains fails when over load is connected and this problem is common in now days. Here is the
simple circuit using optocoupler Digital Mains failure and resumption alarm, for indicating AC mains
fails or resumes by producing alarm sound.
Circuit Description of digital mains failure alarm
The circuit digital mains failure alarm is built around optocoupler. The resistor R1, capacitor C1 & C2,
with diode D1 &D2 provide sufficient voltage to glow internal LED of optocoupler. Here the IC2
CD4011 is used as oscillator to generate low frequency of 0.662 Hz to 1.855 KHz controlling with
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preset VR1. Audio sound is generator by timer IC NE555 (IC2). The generated frequencies from IC2
vary from 472 Hz to 1.55 KHz controlling with preset VR2. For sensing mains fails position of switch
SW1 to point 1 and for sensing mains resumption change the position of switch SW1 to point 2.
PARTS LIST
Resistors (all ¼-watt, ± 5% Carbon)
R1, R4 = 1 KΩ
R2, R5 = 10 KΩ
R3 = 22 KΩ
VR1 = 50 KΩ
VR2 = 47 KΩ
Capacitors
C1 = 0.22 µF
C2 = 1 µF/16V
C3, C4 = 10 µF/16V
C5 = 0.04 µF
C6 = 0.01 µF
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C7 = 100 µF/16V
C8 = 470 µF/16V
Semiconductors
IC1 = MCT2E (optocoupler)
IC2 (N1-N3) = CD4011
IC3 = NE555 (Timer IC)
D1, D2, D3 = 1N4001
Miscellaneous
SW1 = SPDT (Single Pole Double Throw) Switch
SW2 = ON/Off Switch
LS1 = 8Ω/0.5W
9V Battery
Circuit Description of twilight lamp blinker Project Option III
APPLICATION OF THIS PROJECT
The entire circuit of twilight lamp blinker is designed and fabricated around LDR (Light Detector
Resistor) and IC CD4093 (IC1). The preset VR1 is used to control brightness. For sensor LDR1 is used
that has a high resistance during night (i.e. dark) and a low resistance at day time (i.e. light). The
NAND gates (N3 and N4) of IC1 is used as oscillator where high input from NAND gate (N1) makes
the output of NAND gate (N2) low and vice-versa. The high at NAND gate N2 result LED1 blinks by
conducting transistor T1 where transistor T1 is the LED driver transistor. For more brightness more
LEDs is connected parallel to LED1.
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PARTS LIST
Resistors (all ¼-watt, ± 5% Carbon) R1 = 10 KΩ/10W
R2 = 1 MΩ/1W
R3 = 100 KΩ
R4 = 100 Ω
VR1 = 100 KΩ
Capacitors
C1 = 0.68 µF/400V
C2 = 100 µF/40V
C3 = 10 µF/35V
Semiconductors
IC1 (N1 – N4) = CD4093
T1 = BC547
D1, D2 = 1N4007
ZD1 = 5.6V/1W
ZD2 = 15V/1W
Miscellaneous
LED1 = Blinker
LDR1 = Light Detector Resistor
Battery = 4.8 V/500 mAh battery pack
SW1 = SPST (Single Pole Single Throw)
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Power Supply for Integrated circuit (ICs) and Microprocessor Project Option IV
APPLICATION OF THIS PROJECT
Since a power supply is a vital part of all electronics systems. Most digital ICS, including
microprocessor and memory ICS, operate on a ± 5-V supply, while almost all linear ICS (op-amps and
special-purpose ICS) require ± 15-V supplies. Therefore, the power supply presented in this section
will have ±5 and ±15 V.
Working of the system
Figure 1-1 shows the block diagram of a typical power supply. The schematic diagram of the power
supply that provides output voltage of ±5-V at 1.0A and ± 15 V at 0.500 A is shown in Figure 1-2. In
this figure two separate transformers are used because they are readily available; however, it is
possible to custom design a single transformer with the same specifications to replace the two. The
supply voltages are obtained from a 26.8-V center-tapped (CT) transformer, and the supply voltages
are obtained from the 12.6-V CT transformer. The output of these secondaries is then applied to the
bridge rectifiers, which convert the sinusoidal inputs into full-wave rectified outputs. The filter
capacitors at the output of the bridge rectifiers are charged to the peak value of the rectified output
voltage whenever the diodes are forward biased. Since the diodes are not forward biased during the
entire positive and negative half-cycle of the input waveform, the voltage across the filter capacitors
is a pulsating dc that is a combination of do and a ripple voltage. From the pulsating dc voltage, a
regulated dc voltage is extracted by a regulator IC.
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Circuit Description
Consider first how the ± 15-V supply voltages are obtained in the circuit of Figure 1-2. The 7815 is a
+15-V regulator, the 7915 is a -15-V regulator, and both can deliver output current in excess of 1.0
A, They will hence perform satisfactorily in the circuit of Figure 1-2 by providing ±15 V at 0.500 A.
However, since the drop-out voltage (Vin – V0) is 2 V, the input voltage for the 7815 must be at least
+17 V and that for the 7915 must be at least — 17 V. This means that the rectified peak voltage
must be greater than +17 V and — 17 V, which in turn implies that the secondary voltage must be
larger than 34 V peak or 24 V rms. The voltage across the center-tapped secondary in Figure 1-2 is
26.8 V rms, thus satisfying the minimum voltage requirement of 24 V rms. Also, the peak voltage
between either of the secondary terminals and the center-tap (ground terminal) is 18.95 V peak,
which is less than the maximum peak voltages of +35 V and -35 V for the 7815 and 7915,
respectively.
Note that the voltages across the two halves of the center-tapped secondary are equal in amplitude
but opposite in phase. During the positive half-cycle of the input voltage, diode D1 conducts and
capacitor C1 charges toward a positive peak value =18.95 V. At the same time, diode D3 is also
conducting; hence capacitor C3 charges toward a negative peak value = -18.95 V. This means that
the voltage across nonconducting diodes D2 and D4 is 37.90 V peak, which implies that the peak-
reverse-voltage (PRV) rating of the bridge rectifiers must be larger than 37.90 V peak or 26.8 V rms.
The PRV rating of the bridge rectifier diodes, also known as a working inverse voltage (WIV), is
specified on the data sheets. The bridge rectifier, MDA200 (Mot0r0la’s rectifier) in Figure 1-2, has a
PRV rating of 50 V, which is higher than needed. This bridge rectifier is, in fact, used here because it
is readily available and more commonly used.
During the negative half-cycle of the input waveform, diodes D2 and D4 conduct and charge
capacitors C1 and C3 toward the peak voltage of 18.95 V with indicated polarities. Note, however,
that the diode pair that conducts during either the positive or negative half-cycle does not do so for
the entire half-cycle. The diodes conduct only during the time when the anodes are positive with
respect to the cathodes. In other words, when the diodes are forward biased, the capacitors are
charged by current pulses. Data sheets give the maximum average rectified current I0max that the
diode can safely handle. For the MDA200,Iomax is 2.0 A. In addition, when the power supply is first
turned on, the initial charging of the capacitor causes a large transient current called the surge
current to pass through the diodes. The surge current IFS flows only briefly and is therefore much
larger than the maximum average current I0max. The maximum surge-current IFSM is normally
included on the data sheets; it is 60 A for the MDA200.
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Finally, the size of the filter capacitor depends on the secondary current rating of the transformer. As
a rule of thumb, a 1500-µF capacitor should be used for each ampere of current. The working
voltage rating (WVDC) of the capacitor, on the other hand, depends on the peak rectified output
voltage and must be at least 20% higher than the peak value of the voltage it is expected to charge
to. Capacitors C1 and C3 satisfy these requirements (see Figure 1-2). Capacitors C2 and C4 at the
output of 7815 and 7915 regulators, respectively, help to improve the transient response and should
be in the range of 1µF.
Next consider the ±5-V supply. The circuit arrangement of the ±5-V supply is identical to that of the
±15-V supply except that here the specifications for the transformer T2 secondary are different.
Therefore, the operation and considerations for the ±5-V supply are the same as those presented for
the ±15-V supply.
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The voltage regulators in Figure 1-2 will require heat sinks. Let us examine why. The power
dissipated by the 15-V regulators is as follows:
Power dissipated = (dropout voltage) (current) = (18.95 — I5) (0.5) = 1.98 W
Similarly, the power dissipated by the 5-V regulators is (8.91 – 5)(1.0) = 3.91 W
Therefore, for the proper operation the regulators must be heat-sinked in order to keep their
temperature down. If a regulator is a metal package (TO-3 type), the appropriate heat sink is
mounted on the case of the package. However, if the regulator is an epoxy package, silicon grease
may be used on the back of the package, and then the package can be bolted to the chassis of the
power supply cabinet with insulating hardware.
Besides the ±15 and ±5-V regulated supply voltages, there is often a need for a 60-Hz square-wave
signal, which is used as a time base in scanning the digital displays and as a trigger for sequential
and timing circuits. If needed, a 1-Hz (1-s) signal for the real-time clock can be readily obtained
from the 60-Hz signal by using a divide-by-60 network. Although not commonly done, a higher-
frequency Signal can also be obtained from the 60-Hz signal by using e multiplier. For these reasons,
in Figure 1-2 a 60-Hz square-wave signal is produced by using two small-signal diodes and a 555
timer as the Schmitt trigger
PARTS LISTS
Resistors (all ¼-watt, ± 5% Carbon)
R1 = 10 kΩ
Capacitors
C1, C3 = 1500 µF
C2, C4, C6, C8 = 1 µF
C5, C7 = 3000 µF
Semiconductors
IC1 = MC7815
IC2 = MC7915
IC3 = MC7805
IC4 = MC7905
IC5 = NE555 timer
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D1 – D2 =MDA200 PVR = 50 V, I0max = 2.0 A, IFSM = 60 A
D5 – D8 = MDA970A1 PVR = 50 V, I0max = 4.0 A, IFSM = 100 A
D9, D10 = 1N914 signal diodes
Miscellaneous
Transformer T1 = Primary: 117 V, 60 Hz: Hobart P-300
Secondary: 26.8 V CT, 1.0 A
Transformer T2 = Primary: 117V, 60 Hz: Hobart P-305
Secondary: 12.6 V CT, 2.0 V
Fuse 0.750 A slow blow
Switch On-off toggle type
Silicon grease with insulating hardware or four het sink for Voltage regulator
Electronics Cricket on board Project Option V
This is very interesting project not for only who love cricket for also who love to watch this game
because thousands of us want to play this game but some time it is not possible because of this busy
life, lack of ground etc. The game electronics cricket on board can be played by anyone even in their
home by sitting on table. The interesting fact is even a single player can play this game.
Circuit description of electronics cricket on board
This electronics game circuit cricket on board is design by most popular IC LM555 and decade
counter IC CD4017 from CMOS family. IC1 555 timer IC, forms the heart of circuit used as clock
pulse generator. Generated clock pulse is fed to pin 14 of IC2 CD4017. Output is obtained from pin
number 3, 2, 4, 7, 10, 1, 5, 6, 9, 11 by connecting LED to each pin as shown in circuit diagram. To
play this game switch SW1 are placed in on position (or pushed). All 10 LEDs are in on mode. But
when we release switch SW1 last pulse only lit up one LED which is the game result. Now compare
the result of cricket on board to chart and write your score in score boards, lastly count your all run.
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PARTS LIST
Resistors (all ¼-watt, ± 5% Carbon)
R1, R2, = 10 KΩ
Capacitor
C1 = 0.1 µF/50V
Semiconductors
IC1 = NE555 Time IC
IC2 = CD4017
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GAME RESULT
Catch Out LED 1
Stamp Out LED 2
Bold Out LED 3
Leg By LED 4
Single Run LED 5
Two Run LED 6
Four Run LED 7
Sixer LED 8
Wide Ball LED 9
No Ball LED 10
Electronics Lucky Number Project Option VI
The circuit is simple and self-explanatory. IC1, a NE555 timer, is used as astable mode to generate
clock pulses at a rate of about 20 Hz. The frequency can be varied with the help of potentiometer
VR1.
The clock pulses from the timer are fed to clock input of IC2, a decade counter. The outputs of the
counter are decoded by IC3, (BCD to seven segment decoder/driver) which drives a common anode
display (DIS1) to show from figure 0 to 9.
On pressing switch SW1, IC1 starts working, with the display changing from 0 to 9. Capacitors C1 is
charged during this time.
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Once SW1 is released, the capacitor discharges through resistor R3, VR1, R1 and R2. Thus, the
frequency of IC1 decrease (and hence the rate of changing figures on the display) and ultimate
becomes zero, once C1 has totally discharged thereby stopping the displayed is enhanced by the time
for which SW1 is pressed. So, the random effect is natural outcome.
PARTS LIST
Resistors (all ¼-watt, ± 5% Carbon)
R1 = 100 KΩ
R3 = 1 KΩ
R4 – R10 = 330 Ω
VR1 = 100 KΩ
Capacitors
C1 = 47 µF/10V
C2 = 0.47 µF
C3 = 0.01 µF
Semiconductors
IC1 = NE555
IC2 = 7490
IC3 = 74247
D1 = 1N4001
DIS1 = FND507 or LTS542
Miscellaneous
SW1 = push to on switch
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Programmable electronics dice project Option VII
Dice game is very interesting indoor game mostly played in childhood. Here is verified game
project programmable electronics dice useful in many game. With the help of this project we can
display any number between 1 - 9 according to our dip switch setting
Circuit description of programmable electronics dice
The project programmable electronics dice comprises three ICs as heart and for output a common
anode display. Here, IC1 used is a dual 4-input Schmitt trigger NAND gate IC where gate N1 used as
frequency generator which generate the clock frequency of 70kHz with the help of resistor R2 and
capacitor C1 and gate N2 load data at the input of IC2, Where IC2 is a presettable binary counter with
the facilities of parallel loading. Lastly the output of IC2 is displayed on common-anode, 7-segmant
display with the help of IC3 which is BCD-to-7-segmant decoder and the resistor R8 is used as
current limiter.
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Setting for the 4-way DIP switch for display range
Dice Range Close the inner switch Open the inner switch
1 to 2 B and A D and C
1 to 3 C only A, B and D
1 to 4 A and C B and D
1 to 5 B and C A and D
1 to 6 A, B and C D only
1 to 7 D only A, B and C
1 to 8 A and D B and C
1 to 9 B and D A and C
PARTS LIST
Resistors (all ¼-watt, ± 5% Carbon)
R1 = 1 KΩ
R2 = 100 Ω
R3 – R7 = 4.7 KΩ
R8 = 220 Ω
Capacitor
C1 = 0.1 µF
Semiconductors
IC1 = 74LS13, dual 4-input Schmitt trigger NAND gate IC
IC2 = 74LS191, presettable binary counter with parallel facility
IC3 = 7474, BCD-to-7-segmant decoder
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Miscellaneous
DIS-1 = LTS542 common anode display of equivalent
SW1 = ON/OFF switch
SW2 = 4-way dip switch