Tuesday, 28 January 2014

Sensitive Optical Burglar Alarm

This optical burglar alarm uses two 555 timer ICs (IC1 and IC2). Both the ICs are wired as astable multivibrators. The first astable multivibrator built around IC1 produces low frequencies, while the second astable multivibrator built around IC2 produces audio frequencies.
General-purpose Darlington photo-transistor T1 is used as the light sensor. To increase the sensitivity of the circuit, NPN transistor T2 is used.
Place phototransistor T1 where light falls on it continuously. Phototransistor T1 receives light to provide base voltage to transistor T2. As a result, transistor T2 conduct to keep reset pin 4 of IC1 at low level. This disables the first multivibrator (IC1) and hence the second multivibrator (IC2) also remains reset so the alarm (LS1) does not sound.
When light falling on Darlington phototransistor T1 is obstructed, transistor T2 stops conducting and reset pin 4 of IC1 goes high. This enables the first multivibrator (IC1) and hence also the second multivibrator (IC2). As a result, a beep tone is heard from speaker LS1. The beep rate can be varied by using preset VR1, while the output frequency of IC2 can be varied by using another preset VR2.
This circuit works off a simple 6V-12V DC power supply.
PARTS LIST
Resistors (all ¼-watt, ± 5% Carbon unless stated otherwise)
R1, R5 = 1 KΩ
R2 = 100 KΩ
R3 = 4.7 KΩ
R4 = 10 KΩ
VR1 = 1 MΩ
VR2 = 100 KΩ
Capacitors
C1 = 1 µF/16V
C2 = 0.01 µF
C3 = 0.047 µF
C4 = 0.01 µF
C5 = 47 µF/25V
Semiconductors
IC1, IC2 = NE555
T1 = 2N5777 Photo Transistor
T2 = BC547
LED1 = RED LED
Miscellaneous
LS1 = 8Ω / 0.5W

Monday, 27 January 2014

1.5V 555 LED Driver Experiment

This 1.5V 555 LED driver is more of a fun learning experiment than a practical circuit. While the TLC555 can indeed drive a 3V white LED using the inductive discharge technique, it typifies the kind of problems present in low voltage circuits. Two circuits are presented: Basic 555 LED Driver and Bootstrapped 555 LED Driver.
Circuit function

When the output (pin 7) goes low, it charges L1 and when it turns off, the voltage developed by the inductor discharge easily causes the voltage across the LED to increase to its threshold voltage and subsequently flow through the LED.

Bootstrap mode

Note that operation of the toggle switch is necessary to shock the device into oscillation at marginally low voltages – otherwise, it cannot start. What happens is that when the switch closes, C2 charges through L1 and rings up double the incident input voltage – this is the effect of series resonance. Rectifier D2 and capacitor C2 then hold Vcc at a higher voltage level until oscillation commences and L1 starts repetitively firing the LED at 3V thus keeping C2 charged. This is a very interesting part of the experiment.

Not all 555s are created equal

To make this LED driver circuit function, the 555 must operate well below the specified minimum Vcc. Also, the maximum voltage specification of the open collector output (pin 7, discharge function) is not specified in relation to Vcc (pin 8). The first TLC555 worked so poorly under these conditions that I decided not to use its data. The particular LM555 was selected because I knew that it functioned OK at very low voltages. So a word for the wise – whoever attempts to replicate any of this stuff, will need a bag of 555s.

Results, Fig 1

Minimum voltage TLC555: 1.36V (some LED current as low as 1.0V – self-starting @ 1.0V)
Minimum voltage LM555: 2.30V (no LED current below this point – self-starting @ 2.3V)

Results, Fig 2, bootstrap mode

Minimum voltage TLC555: 1.13V (some LED current as low as 0.56V, self-starting @ 1.1V)
Minimum voltage LM555: 1.78V (some LED current as low as 0.80V, self-starting @ 2.5V)

Datasheet ZXSC380 (for comparison – I did not actually test this device)

Minimum startup and operating voltage: 0.9V typical, 1.0V max

Muting Transistor Attenuator Circuits and the 2SC2878

Among semiconductors, the muting transistor and its audio application is perhaps the most obscure and poorly understood of all. There is extremely little information on this subject available on the internet and what is available is sketchy. This discussion is an attempt to tie the pieces together and to add some insight –I have been working on this off and on for some time and for me it has been a learning experience. While I do not claim expertise in this subject, I question if such experts actually exist.
Applications for muting circuits
Applications for muting circuits abound. Included are synthesizers, audio amplifiers, pre-amplifiers, audio mixers and audio line & level equipment (both consumer and professional). In amplifiers and pre-amplifiers, the muting circuit is intended to prevent the popping of loudspeakers when power is applied. In mixers and audio line & level equipment, the muting circuit may also be employed to select /deselect various input channels –such must be done cleanly or quietly.
Types of muting circuits
Obviously, the function of muting circuits is to mute (kill) the audio signal. This can be done in a number of ways including switches, relay contacts, junction FETs, analog switches and bipolar muting transistors. Switch and relay contacts can be noisy and intermittent due to contact bounce. Furthermore, properly applied contacts must be dry circuit rated due to both the low current and potential across the contacts –this forces the use of bifurcated dry circuit contacts that are special and expensive. While a junction FET is sometimes applied as a variable attenuator, its use as a muting device is a misapplication due to the lack of symmetry because it cannot support more than about 600mV due to its intrinsic body diode. Analog switches can do the job if applied correctly, but lack the audio range required in professional line and level applications, may be subject to crosstalk between sections and are also very sensitive to ESD. On the other hand, the bipolar muting transistor does everything well and inexpensively.
What is unique about the bipolar muting transistor?
The standard NPN transistors is symmetrical in that it consists of 3 layers, 2 layers of “N” material (collector & emitter) separated by a layer of “P” material (base). However, that is as far as the symmetry goes as the layer thicknesses and doping varies greatly. The standard transistor still functions with the collector and emitter terminals reversed, but the hFE (current gain) in this mode is reduced by perhaps two orders of magnitude and the reversed voltage rating (Vebo) generally limited to about 5V.
In comparison, the muting transistor is a good deal more symmetrical –it has high reverse hFE and some types offer a 15 to 40V base to emitter reverse voltage rating (Vbeo). In effect, it is rated for AC operation and this suits it well for audio voltage signals that are AC in nature. Whichever terminal (emitter or collector) is the most negative becomes the effective emitter terminal. If sufficient base drive is applied, it will saturate either polarity, and this is exactly what is required to implement the mute function.
Two categories of muting transistors
The two categories are graded by the base to emitter reverse voltage rating (Vbeo).
The 1st category Vbeo is limited to 5V and is suited for consumer electronics that has an average program signal level of -7.8dbu (0.315Vrms or 0.445Vpeak). A 5V rated device provides 21db headroom to handle program material transients.
The 2nd category Vbeo starts at 15V and is suited for professional studio line and level devices that have an average program signal level of +4dbu (1.228Vrms or 1.736Vpeak). A 15V rated device provides 18.7db headroom to handle program material transients.

BBC NEWS

ARY NEWS


Sunday, 26 January 2014

NATIONAL GEOGRAPHIC



GEO NEWS


WATCH




555 Amplifier Circuit

The 555 can be used as an amplifier. It operates very similar to pulse-width modulation. The component values cause the 555 to oscillate at approx 66kHz and the speaker does not respond to this high frequency.  Instead it responds to the average CD value of the modulated output and demonstrates the concept of pulse-width modulation. The chip gets very hot and is only for brief demonstrations. 

Knight Rider Circuit


Inverted 555 Timer Circuit

Whenever I use the 555 timer, it seems that the output polarity is invariably incorrect, and the way the 555 functions, it normally cannot generate a duty cycle of less than 50% — 90% yes, 10% NO! This inverted 555 circuit generates duty cycles of less than 50%. Everything works the same except for the polarity. Why not simply invert the output with a transistor? Will not that do the same? Legitimate question… Actually NO, because a transistor that inverts the output cannot provide the desirable totem pole source/sink output function of pin 3. And there is another reason that we will get in the future—this is a 555VCO circuit that requires the inverted timer.
The schematic shows (3) circuits, because one circuit does not work well over the entire Vcc range.
The first simply uses a “normal” 2N3904 garden variety transistor, and this works well when Vcc < 9V. When Vcc > 9V, the base to emitter junction starts to zener and disrupts operation. Transistor base to emitter junction zeners a little above -6V.
The second circuit adds D1 to the emitter of Q1 in order to increase VEBO. With this mod, Vcc may be increased to the 18V limit. However, D1 may be eliminated if we use the special 2SC2878 switching transistor that has a VBEO rating of -25V. These devices are no longer in production, but are available on eBay—every serious experimenter should have a few in his component collection. The types now in production use the tiny SO-23 SMD package.
The third circuit uses a J112 N-Channel JFET for Q1. The JFET is a curious device that works well for the application provided we allow for the VGS(OFF) parameter. VGS must be less than Vcc /3. (e.g. if Vcc = 9V, VGS(OFF) must be less than 9V /3 or 3V for proper operation). Since the VGS(OFF) parameter is sloppy (-1 to -5V), the device must be selected—to the left is a simple test circuit—actually, most devices will work OK. The J112 should also be in every serious experimenter’s component collection.
How it works
You will note that C1 is tied to Vcc rather than common and that R1 & R2 charge it in the negative direction. By connecting C1 to Vcc, the relatively high discharge current does not run through the power source. The reset transistor (Q1) discharges the capacitor in the positive direction. R1 & R2 are determined in the same fashion as the normal 555 timer. R3 is a pull-up resistor for the open collector output (pin 7) so it can drive the emitter follower (or source follower) reset transistor.
R1 scales the output frequency—here it is about 1.25kHZ and it can be rescaled to whatever you need.
R2 controls the reset pulse width for low duty cycle (short output pulse) output—the larger it gets, the more it affects output frequency.
Pin 5 does not need a bypass capacitor unless you desire high stability generally I omit this capacitor.

Temperature Alarm Circuit

This simple Over heat alarm is to monitor heat generating devices such as motor, inverter etc. The alarm will beep and LED blinks when the temperature of the device increases abnormally.
The circuit is a simple Astable multivibrator using the low power CMOS timer IC 7555 which is the low power version of the popular 555 IC. The reset pin 4 of IC1 is used to activate the alarm. The astable will work only if the reset pin 4 becomes high. The reset pin is connected to the positive rail through the 10 K NTC thermister. The NTC (Negative Temperature Coefficient) thermister offers high resistance in cold and its resistance becomes low to few ohms when the temperature in its vicinity increases. So when the temperature is low (as adjusted by the position of the thermister near the device) reset pin of IC1 remains low and astable is in off position and buzzer remains silent. When the temperature near the thermister increases, its resistance decreases and provides voltage to the reset pin of IC1 and the astable starts working.
Note: Fix the thermister near the device by adjusting the distance between the thermister and the heat generating area of the device so as to keep the alarm silent when the heat is normal.


Digital signal processing (DSP) Practical


EMBEDDED SYSTEM

Embedded systems
Examples of Embedded systems
Technology for Embedded systems
Microprocessor vs Microcontrollers
Microcontroller Families
Criteria to choose a microcontroller
Overview of 8051 family
Applications/ Some projects

TRW&PS

Important Presentation Characteristics
• Purpose
o Be clear about the message that you are trying to convey.
• Audience
o Know your audience and their level of understanding.
o Make your presentation appropriate to their interests & level of
understanding.
o Make it interesting.
• Approach
o Make it easy for your audience to agree with your message.
• Time Limit
o Do not exceed the time limit.
o To know how long your presentation will run you must practice.
o Do not move any faster than one slide per minute.

Sunday, 12 January 2014

Learning Physics Modeling with PhysX


Book Description
In this day and age, physics engines play a very critical role in the success of a sophisticated game. PhysX is a state-of-the-art cross-platform physics engine widely used by top game studios and developers. It contains all the physics-related components you will need and exploits the parallel-processing capability of modern GPUs as well as multi-core CPUs to make a game as physically-realistic as possible. This book will help you to program and simulate games by using PhysX 3.

Learning Physics Modeling with PhysX helps you to master physics simulation using the PhysX Physics Engine from scratch. This is useful not only for game developers, but also for developers making virtual walkthroughs or training and other simulation applications. It will cover all the essential features of PhysX 3 with easy-to-understand code snippets and examples to help you learn quickly and efficiently.
Book Details
Publisher: Packt Publishing
By: Krishna Kumar
ISBN: 978-1-84969-814-6
Year: 2013
Pages: 104
Language: English
File size: 3.7 MB
File format: PDF

A Peek at Computer Electronics


Book Description
Are you a programmer or computer enthusiast? Do you feel comfortable with methods, functions, and variables? Do you wish you knew more about how the computer made it all work? Now you can. From basic electronics to advanced computer hardware, you'll learn the magic behind the gear that makes it all run.

If you're into tinkering, or ever thought about it, this book explains the basics of how it all works.
Book Details
Publisher: The Pragmatic Programmers
By: Caleb Tennis
ISBN: 978-0-9776-1668-8
Year: 2007
Pages: 250
Language: English
File size: 5.52 MB
File format: PDF

Make: Arduino Bots and Gadgets

Book Description
Want to build your own robots, turn your ideas into prototypes, control devices with a computer, or make your own cell phone applications? It's a snap with this book and the Arduino open source electronic prototyping platform. Get started with six fun projects and achieve impressive results quickly.

With Arduino, building your own embedded gadgets is easy, even for beginners. Embedded systems are everywhere - inside cars, children's toys, and mobile phones. This book will teach you the basics of embedded systems and help you build your first gadget in just a few days. Each learn-as-you-build project that follows will add to your knowledge and skills.
Book Details
Publisher: O'Reilly Media
By: Tero Karvinen, Kimmo Karvinen
ISBN: 978-1-4493-8971-0
Year: 2011
Pages: 296
Language: English
File size: 55.7 MB
File format: PDF

Make: Electronics

Book Description
Want to learn the fundamentals of electronics in a fun, hands-on way? With Make: Electronics, you'll start working on real projects as soon as you crack open the book. Explore all of the key components and essential principles through a series of fascinating experiments. You'll build the circuits first, then learn the theory behind them!
Book Details
Publisher: O'Reilly Media
By: Charles Platt
ISBN: 978-0-596-15374-8
Year: 2009
Pages: 360
Language: English
File size: 17.9 MB
File format: PDF

Comodo Dragon Internet Browser 24.0



Comodo Dragon is a Chromium technology-based Browser that offers you all of Chrome's features PLUS the unparalleled level of security and privacy you only get from Comodo. Including a greater level of privacy than Chromium technology offers.
Features:
Improved Privacy over Chromium
Easy SSL Certificate Identification
Fast Website Access
Greater Stability and Less Memory Bloat
Incognito Mode Stops Cookies, Improves Privacy
Very easy to switch from your Browser to the Dragon.

uTorrent 3.3 Beta 28918

µTorrent is a small and incredibly popular BitTorrent client.
Micro-Sized Yet Feature Filled
Most of the features present in other BitTorrent clients are present in µTorrent, including bandwidth prioritization, scheduling, RSS auto-downloading and Mainline DHT (compatible with BitComet). Additionally, µTorrent supports the Protocol Encryption joint specification (compatible with Azureus 2.4.0.0 and above, BitComet 0.63 and above) and peer exchange.
Resource-Friendly
µTorrent was written with efficiency in mind. Unlike many torrent clients, it does not hog valuable system resources - typically using less than 6MB of memory, allowing you to use the computer as if it weren't there at all. Additionally, the program itself is contained within a single executable less than 1 MB in size.
Skinnable and Localized
Various icon, toolbar graphic and status icon replacements are available, and creating your own is very simple. µTorrent also has support for localization, and with a language file present, will automatically switch to your system language. If your language isn't available, you can easily add your own, or edit other existing translations to improve them!

Google Chrome 26.0.1386.0 Dev

Google Chrome is a browser that combines a minimal design with sophisticated technology to make the web faster, safer, and easier.
One box for everything
Type in the address bar and get suggestions for both search and web pages.
Thumbnails of your top sites
Access your favorite pages instantly with lightning speed from any new tab.