Archive for the ‘Coreelectronics’ Category

Stereo Synthesizer

December 30th, 2010 by Thomson | No Comments | Filed in Coreelectronics

There are two common methods of producing a pseudo stereo effect from a mono signal, playing the mono signal from the two speakers in antiphase, and the use of frequency selective techniques which normally consists of directing lower frequency signals into one channel and higher fre­quency signals into the other. This circuit uses the second technique, but can additionally give antiphase signals which can give a better effect, especially when using headphones.

stereo synthesizer Stereo Synthesizer

stereo_synthesizer

Q1 is used as an emitter fol­lower buffer stage which ensures that the two filter networks fens from its output are driven from a low impedance source. If these were driven direct from the input, it is quite possible that they would be fed from a source impedance of a few kilo ohms or more, which would be quite sufficient to alter their effective characteristics.

The two filters are formed by R4 and C3 (low pass), and C6 plus R8 (high pass). A high roll off rate is by no means essential in this application and the 6dB per octave attenuation rate of simple RC filt­ers such as these is perfectly ade­quate. The -3dB point of each filter is at approximately 800Hz and the combined output of the filters, therefore, gives a virtually flat res­ponse with no significant peaks or troughs.

Q2 is connected as an emitter follower buffer stage and this ensures that there is minimal loading on the low pass filter. Q3 similarly ensures that there is minimal load­ing on the high pass filter, but this device is also used as a phase splitter. With SW2 switched to take the output from Q3’s emitter, Q3 effectively operates as an emit­ter follower and gives no phase inversion. With SW2 switched to take the output from Q3’s col­lector, Q3 then effectively acts as a common emitter stage with 100% negative feedback (and unity voltage gain) due to R11. 1t also provides a 180° phase shift so that the two output signals are in anti-phase. An in-phase relationship is needed to give a good central ste­reo image and the use of anti-phase signals tends to give an im­pression of increased channel separation.

In a stereo orchestral recording, it is normal for the violins to come from the left hand channel, with the cellos and basses from the right hand channel. Therefore, the high frequency signals are fed to the left channel and the low fre­quency signals are fed to the right channel so that the unit provides a similar effect (although it will ob­viously function properly with the outputs connected either way).

Broad Band Wireless Communication Systems

November 9th, 2010 by Thomson | No Comments | Filed in Coreelectronics

Wireless communication has experienced tremendous growth in the last decade. High data rate wireless communication is becoming increasingly important to mobile users in corporate and public networks in the indoor environment. Although voice and low data rate services were the first applications of cellular networks, the focus in recent years has shifted to very high-bandwidth delivery, which is a key driver for system and network design. While wireless local area (WLAN) access is important for data applications, mobile users still expect reliable GSM and 3G coverage for their voice service and seamless transition as they move indoors from an outdoor environment. Research shows that 75% of all mobile calls originate inside buildings at work, home or public places. This has in turn led to consumer awareness and expectation of ubiquitous coverage, and the ability to use their wireless devices anywhere.

 Relying on the penetration of the GSM and 3G radio signals from the outside for providing in-building coverage is neither practical nor reliable in many buildings, and additional indoor antenna units (AUs) must be installed. Different building shapes and materials such as steel and metalized glass, cause in-building penetration of radio frequency (RF) signals to weaken resulting in reduced data rates and even complete loss of signal. This will become even more apparent over the next few years with the introduction of new 4G technologies which require considerably higher signal integrity and radio frequency than their voice counterpart. Also, with the trend to increasing data rates on wireless networks and a rapidly increasing number of users who want un-tethered access pose new challenges to system integrators and network designers. This results in significant challenges for the wired infrastructure that is required to connect the numerous antennas units.

 Wireless over fibre (WoF) systems which also known as Radio over Fibre (RoF) systems have attracted much interest for broadband wireless access, offering a simplified  overall system design due to the aggregation of RF signal generation and network management at a central location. Distributing broadband wireless signals over optical fibre has a number of advantages compared with traditional copper cabling. The wide bandwidth of optical fibre further allows different services such as Gigabit Ethernet, IEEE802.11a/g, GSM and 3G to share the same infrastructure, making the wireless-over-fibre approach a truly multi-operator and multiservice technology.

WLANs have had a profound impact on our perception of communication. First of all, the vast majority of users now believe in the new notion of “always on” communication. We are now living in the era of ubiquitous connectivity or “communication anytime, anywhere, and with anything”. Secondly, the concept of broadband communication has caught on very well. As fibre penetrates closer to the end-user environment (Fibre to the Home/Curb/X, FTTH/C/X), wired transmission speeds will continue to rise. Transmission speeds such at 100 Mbps (Fast Ethernet) are now beginning to reach homes. The demand to have this broadband capacity also wirelessly has put pressure on wireless communication systems to increase both their transmission capacity, as well as their coverage.

Broad Band Wireless Communication Systems Broad Band Wireless Communication Systems

Figure 1: PRESENT COMMUNICATION SYSTEMS

In general there is a trade off between coverage and capacity. Figure 1 shows the relationship between some of the various standards (present) in terms of mobility (coverage), and capacity. For instance, the cell size of Wireless Personal Area Networks (WPANs) is typically a few metres (picocell), while their transmission rates may reach several tens of Mbps. On the other hand 2G (e.g. GSM), and 3G (e.g. Universal Mobile Telecommunication System (UMTS) and the International Mobile Telecommunications (IMT2000)) systems have cells that extend several kilometres, but have data rates limited to less than 2 Mbps. Therefore, as mobile communication systems seek to increase capacity, and wireless data systems seek to increase coverage, they will both move towards convergence. A case in point is the IEEE 802.16, otherwise known as WiMAX, which appears to lend weight to the notion of convergence, as shown in Figure 1 WiMAX   seeks  to  provide  high-bit  rate mobile services  using  frequencies  between      2-11 GHz. In addition, WiMAX also aims to provide Fixed Wireless Access (FWA) at bit-rates in the excess of 100 Mbps and at higher frequencies between 10 – 66 GHz.

Toshiba Satellite L300

October 30th, 2010 by Thomson | No Comments | Filed in Coreelectronics
toshiba satellite l300 150x150 Toshiba Satellite L300

Toshiba Satellite L300

Sometimes we get a notebook that packs so much punch into an affordable platform that makes us wake up and actually take notice. And this is the case with Toshiba Satellite L300D – 01N Laptop computer. Big name but small price!

This Satellite L300 laptop from Toshiba is well within an affordable price range, but it still packs all the useful components you need to get your life fun around.

What it has is Dual Core processing, Wireless connectivity and much more.

Processor

Toshiba Satellite L300 runs on AMD Athlon 64X2 Dual-Core QL-60 1.9 Ghz Processor. This CPU gives you processing speeds of 1.9 Ghz per core.

Memory

AMD Athlon 64X2 Dual-Core QL-60 1.9 Ghz Processor of Toshiba Satellite L300 is backed up by 2GB of DDR2 memory. This will knock out memory hungry applications easily. As well as making multi tasking operations.
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Mobile phone battery saving tips

September 9th, 2010 by Thomson | No Comments | Filed in Coreelectronics

Mobile phones have become an integral part of our life. It has influenced our lives in such a way that we cannot even live without mobile phones. Since it is a battery operated device, we expect maximum hours of operation after a battery recharge. You can make sure that your mobile phone will not become dead due to low battery, if you follow the simple steps furnished below.

One of the major causes for sudden battery drain is nothing other than playing games. This fact might make you unhappy, but if you are going to a place where there is not facility to charge your mobile phone you can think of not playing games.

If you are sure that you are not going to make any calls and there is no chance for an incoming call, then switch off your mobile phone without a second thought. Thing is that, we usually keep our phones in our coat or bag in the switched on state, even when we are sure that we don’t need mobile phones for a specific time period.

If you are in an area of weak signal strength, more battery charge will be utilized, while your mobile phone searches for signal. So you can think of switching off your mobile phone if you are sure that you will be in an area of weak signal strength for a long period of time. At the same time less battery charge is used when your mobile phone searches in a strong signal condition.

You can get more out of your mobile phone battery if you turn off the backlight and vibrate function. Ringing takes less power as compared to vibrate function.

Limited net surfing can save battery charge. Sensible use of Bluetooth will definitely help you to save battery charge.

Telephone Amplifier

April 7th, 2010 by Thomson | No Comments | Filed in Coreelectronics

A telephone amplifier enables more than one person to follow a telephone conversation. The unit described here, in common with all normal units of this type, requires no direct connection to the telephone. Instead, the special pick-up coil has a built-in rubber suction cap that enables it to be easily attached to the telephone base. This produces a very weak signal from the magnetic field radiated by an inductive component inside the telephone, but satisfactory results can be obtained if it is fed to low noise, high gain amplifier. It would of course be possible to use a much simpler circuit if a direct connection to the telephone were to be made, but this would make installation more difficult and it is ILLEGAL to make a direct connection to a Post Office telephone anyway.

Telephone amplifier Telephone Amplifier

The preamplifier stage of the unit is based on IC1 which is a low noise op amp having a FET input stage. This is used in the conventional inverting audio amplifier mode and the negative feedback network, R1, 4, sets the voltage gain at about 40dB. (100 times C11 reduces the gain slightly at high frequencies in order to obtain an improved signal to noise ratio.

C4 couples the output from the preamplifier to volume control, RV1, and from here the signal is coupled to the power amplifier by C5. The output stage uses the TBA820M, a class B amplifier which will give an output power of a few hundred milliwatts rms. The closed loop voltage gain of the device is determined by the value of R6, about 25dB. (180 times) with the specified value. This gives the required very high overall gain in conjunction with the preamplifier’s gain. C7, R7 and C8 are needed in order to maintain stability.

The quiescent current consumption of the unit is only about 5mA, but this rises to as much as 50mA or so at high volume levels. The best position for the pick-up coil on the telephone base (not the handset) can be located with a little experimentation.

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VMOS 10 Watt Amplifier

April 6th, 2010 by Thomson | No Comments | Filed in Coreelectronics

At first sight this circuit may seem to be a straightforward Class B design having an emitter follower, complementary output pair and Darlington Pair common emitter drive stage. However, the output devices are, in fact, complementary VMOS transistors used in the source follower mode (the FET equivalent of the emitter follower).

VMOS 10 watt amplifier free projects VMOS 10 Watt Amplifier

R1 and R2 are used to bias the unit to give the optimum quiescent output potential and they provide overall negative feedback, which improves the quality of reproduction. D1 and C4 are boot strapping components, enabling the gate drive voltage to Q3 to go above the positive supply potential, giving improved efficiency to the circuit. R3 is the main collector load for Q2 and PR1 is used to give a standing bias on the output transistors that gives a quiescent current consumption of about 25mA. The thermal compensation circuitry normally used is totally unnecessary in this circuit, since VMOS devices do not suffer from thermal runaway. In fact the quiescent bias current will drop slightly as the output devices heat up, but not sufficiently to give rise to significant crossover distortion.

C2 and C5 provide DC blocking at the input and output respectively, while C1 is a supply decoupling component. C3 gives a degree of high frequency attenuation and aids the stability of the circuit.

Although the current in the driver stage, only about 1mA, may seem to be totally inadequate, it is in fact more than sufficient since the VMOS devices have extremely high input impedances and consume no significant, input current. This is one of their main advantages over bipolar devices. One disadvantage in this particular application is lower efficiency due to the higher threshold voltages and on resistance of VMOS transistors in comparison to bipolar devices. However, the circuit will give an output of 10W rms using a supply voltrage of about 33V or so (with a current drain of up to about 600mA). An input of about 500mV rms is needed for maximum output.

Note: The output devices do not have internal zener protection diodes and the appropriate handling precautions should be taken.

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Cassette Preamplifier

April 3rd, 2010 by Thomson | 1 Comment | Filed in Coreelectronics

Used in conjunction with one of the cassette mechanisms currently available on the surplus market (or a mechanism removed from an old recorder or player) this preamplifier circuit makes an inexpensive but useful cassette player for use with a hi-fi system.

The output signal level from a cassette tape head is typically about 500 micro Volt or so at middle audio frequencies for a mono head and about half this level for a stereo type. The preamplifier must, therefore, provide a considerable amount of voltage gain in order to match this to a hi-fi amplifier, since these require a signal level about 1,000 times higher. It is also necessary for the preamplifier to provide equalization, because the output from a tape head rises at a rate of 6dB per octave. However at higher audio frequencies, tape heads are not very efficient and require a much less rolloff.

free electronics projects cassete preamplifier Cassette Preamplifier

Q1 and Q2 are used in a conventional two stage, direct coupled, common emitter amplifier and the frequency-selective negative feed-back through C3 and R4 provides the appropriate equalization. These also set the midband voltage gain of the input stage at about 46dB. With such a low input level it is obviously necessary to use low noise transistors (Such as the BC109C) in order to obtain good results. Running Q1 at a low collector Current, about 200uA, also helps.

Q3 is used as a low gain common emitter stage, which provides the additional amplification. R9 introduces negative feedback, which controls the voltage gain of Q3 and the specified value gives a gain of about 14dB. For a stereo unit R9 should be reduced to 390R in order to give increased gain, to compensate for the lower output of a stereo tape head.

When playing a Dolby B encoded cassette SVV1 can be closed; this gives a small degree of treble cut which provides a reasonably flat overall response.

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Scratch and Rumble Filter

March 18th, 2010 by Thomson | No Comments | Filed in Coreelectronics

This is a 12 dB per octave add-on scratch and rumble fill-r which can be connected into the ‘tape Monitor’ or some similar facility of the amplifier.

It is a conventional second order filter circuit having passive high pass filter formed by the series capacitance C3 and C4, plus the parallel resistance of R2 and R3 (the latter also being used to bias emitter follower transistor Q1). A passive filter of this type gives only a very slow initial roll off, and an ultimate attenuation rate of only 6 dB per octave. A bootstrapping resistor is therefore used to improve performance. Above the cut-off frequency, where the gain of the circuit would otherwise fall off somewhat, R1 has the effect of reinforcing the input signal. Well below the cut off frequency, losses through C4 result in the signal level at Q1 emitter being well below that at the junction of C3 and C4. This results in some of the signal at the junction of C3 and being tapped off through R1, with C3 and R1 effectively forming a second high pass filter network. This eliminates the sluts, initial roll off rate (in fact there is a small and insignificant peak of about 0.5dB above the cut off frequency) and speeds up the attenuation rate to a nominal 12dB per octave.

sceatch and rumble filter 300x141 Scratch and Rumble Filter

The low pass filter works in much the same way as the high pass one, except of course, the R and C filter elements have been transposed so as to give the correct filter action.

With the specified component values the rumble filter response falls below unity at approximately 45Hz, reaches the -6 d13 point just above 30Hz, and then falls away at a nominal 12dB per octave. The scratch filter response crosses the unity gain point at about 6k5Hz, reaches the -6dB point at approximately 10kHz, and then falls away at a nominal 12dB per octave.

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Simple amplifier

March 17th, 2010 by Thomson | No Comments | Filed in Coreelectronics

The term “amplifier” covers a very wide range, from a one transistor preamp to an ultra sophisticated high power hi-fi system. There is little doubt that the circuit shown here is very simple. The output is in the order 250mW – quite sufficient for most purposes and comparable to that of the average transistor radio. The distortion level is rather high, being about 5%.

The amplifier is also reasonably sensitive and will give full output with an input of about 50mV. Input impedance is about 50kR.

free electronic projects simple amplifier 300x227 Simple amplifier

The slider from the volume control is connected to the, base of Q1 via a DC blocking capacitor. Q1 is connected as a conventional common emitter amplifier with R2 provides the base bias and R3 acting as the collector load. This stage is directly connected to the second transistor which is a PNP type. In this way the current passing through Q1 provides the bias for the second transistor. The output of the second transistor is connected directly to the speech coil of the loudspeaker. This is not normally good practice since the standing current in the output transistor continually biases the coil either slightly in or out from its usual operating point. However if a large speaker is used, as it should be, this has very little effect and, since we are not aiming at hi-fi, it does not matter.

The tone control comprises C2 and RV2 which are connected between the collector and base of Q1 At high resistance settings RV2 has little effect but on minimum settings the 100nF feeds back the high frequencies out of phase, thus cancelling them.

For this circuit to work properly, R3 must be selected with great care. The value shown here of 39 ohms is a typical one and, although it may be used for initial setting up to ensure the circuit is operating, the value should be found by experiment. If it is too low there will be severe distortion at higher volume settings. If it is too high the current drain will be excessive even though the quality of reproduction will be good.

It is very important that Q2 is fitted with a heat sink as it will get very not.

The speaker impedance is not all that critical and in the prototype speakers with an impedance as low as 8 ohms and as high as 80 ohms all worked well, although changing the speaker impedance will also necessitate a change in the value of R3.

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Treble booster

March 13th, 2010 by Thomson | No Comments | Filed in Coreelectronics

A treble booster circuit can be used with an electric guitar (and also electronic instruments) to boost the higher order harmonics and give a more brilliant sound. A circuit of this type gives a fairly flat response at bass and most middle audio frequencies, with the upper-middle and lower treble frequencies being given a substantial amount of boost. It is normal to use only a modest amount of emphasis to the upper treble in order to give good stability and a low noise level, and this also prevents the output from sounding too harsh. The frequency response is shown in the accompanying graph.

treble booster free circuit diagram 300x168 Treble booster

The circuit is basically an op-amp used in the non-inverting amplifier mode. The non-inverting input is biased by R4 and R5 via a decoupling network which is comprised of R3 and C3. C4 and C5 give DC blocking at the input and output respectively. With SW1 open there is virtually 100% negative feedback through R1, R2 and C1, giving the circuit unit gain and a flat response. Closing SW1 brings C2 into circuit, and this de-couples some of the feedback through R1 and R2 at frequencies of more than a few hundred Hz, giving the required rising response. Feedback through C1 at high treble frequencies causes the response to fall away above about 5k5Hz, and prevents the very high frequency harmonics from being excessively emphasized.

treble booster frequency response curve 300x264 Treble booster

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RIAA stereo preamplifier

March 13th, 2010 by Thomson | No Comments | Filed in Coreelectronics

Records are cut with a frequency response such that when they are replayed with a magnetic pickup and a preamplifier with RIAA equalization (Recording Industry Association of America) the reproduced sound will be as similar to the original as possible.

The disc is cut at constant amplitude, except from 500Hz to 2120Hz where it is cut at constant velocity. When this disc is replayed with a magnetic pickup, the relative output voltage rises with frequency, due to the fact that the magnetically generated voltage is proportional to the velocity of the stylus as it moves sideways in the groove. To restore the original sound quality, a preamplifier with a frequency response that, gives decreasing output with increasing frequency is required. This response curve is known as the RIAA equalization and it is tailored accurately to fit the cutting and replay processes. The signal level from a magnetic pickup is low, generally 20mVpp and so a low noise pre- amplifier is needed.

RIAA sterio preamplifier left RIAA stereo preamplifier

RIAA sterio preamplifier right 300x181 RIAA stereo preamplifier

The circuit shows a realization of this requirement. The low noise amplifier is the LM381 -made by National Semiconductors. A DC bias control is included (RV1, RV2), and the feedback components generate the RIAA curve. Use screened cable for the wiring to the pickup, keep the circuit away from transformers (and the pickup and its wiring) and connect all the earths together, near to the IC.

RIAA sterio preamplifier graph 300x263 RIAA stereo preamplifier

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Free download manager

March 4th, 2010 by Thomson | No Comments | Filed in Coreelectronics

free down load manager Free download managerDownload manager software can do wonders for people who wish to download a lot of data and files. The main problem with downloading large files is that, there is a chance for the internet connection to break while downloading. If you are using a download manager then the file download will resume when the connection comes back. FDM (Free Download Manager) is one such useful software utility using which you can manage all your downloads. As a download manager FDM is an easy to use tool. FDM is a powerful download accelerator which is free to download at the same time. No need to worry about the safety of FDM, it is hundred percent safe. Since it is open source software, GPL license governs its distribution.

Features of FDM

Unbeatable download speed:

FDM uses the technique of splitting the file being downloaded into sections. After the file has been sliced into different sections, all sections are downloaded at the same time. This increases the download speed up to 600 percentages.

Broken download management:

Oops! Internet connection failed. No need to worry about such a scenario. With FDM broken downloads are automatically resumed. So just start the download and forget it.

Support for protocols:

Files from any remote server can be downloaded using HTTP, HTTPS and FTP. BitTorrent protocol can also be used for file downloads.

Video download support:

Download your favourite videos from your favourite video sites like Google video, YouTube etc. The downloaded videos can be saved in .flv format, or can be converted into other commonly used formats.

How to get FDM?

Follow the below link to download FDM

DOWNLOAD FDM

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Intel atom Z500 price and Intel atom Z500 specifications

February 1st, 2010 by Thomson | No Comments | Filed in Coreelectronics

Intel atom Z500 price and specifications Intel atom Z500 price and Intel atom Z500 specificationsIntel atom Z500 processors are very small processors with a dimension of 13X14 mm. Intel atom Z500 consist of nearly 47 million transistors. Number of transistors that constitute Intel atom Z500 processor is more than the number of transistors used to build up Intel Pentium 4 processor. Level-1 cache of Intel atom Z500 processor is about 56KB. Intel atom Z500 has a level-2 cache of about 512KB. The bus used in association with Intel atom Z500 processor is the same as used along with Intel Pentium 4. Bus frequency is about 400/533 MHz.

Intel atom Z500 Specifications:

Intel atom Z500 has only one core.

Intel atom Z500 has two threads.

2 GHz is the base frequency of Intel 500 processor.

Intel atom Z500 is a 32 bit microprocessor.

Intel atom Z500 has 512 KB of L2 cache.

FSB speed of Intel atom Z500 is about 533 MHz.

Intel atom Z500 Price:

Price of Intel atom Z500 is about 45 dollars. ie 2,083.12 INR

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Intel core 2 duo E6700 Price and core 2 duo E6700 Specifications

January 30th, 2010 by Thomson | No Comments | Filed in Coreelectronics

intel core two duo processor Intel core 2 duo E6700 Price and core 2 duo E6700 SpecificationsAmong all processors now available in the market Intel core 2 duo E6700 is the most cost efficient processor. Since miniaturization is the order of the day processors that can deliver the maximum with the minimum power is preferred by the industry. If the power consumption of a processor is less heat generated by it will also be less. From this point of view Intel core 2 duo E6700 can be given the highest mark. Intel core 2 duo E6700 consume less power compared to other processors available in the market. This low power consumption feature of Intel core 2 duo E6700 points to the fact that the heat produced by Intel core 2 duo E6700 is also less. Intel core 2 duo E6700 is not only a cool processor, it can work without making much noise. All the above mentioned features of Intel core 2 duo E6700 makes it suitable to be used in small PC designs.

Features of Intel core 2 duo E6700:

Intel core 2 duo E6700 is a 64 bit processor.
Clock speed of Intel core 2 duo E6700 processor is 2.66GHz.
Intel core 2 duo E6700 ultra performing processor has a bus speed of 1066MHz.

Price of Intel core 2 duo E6700:

Price of Intel core 2 duo E6700 is 397.95 dollars. ie 18,413.15 Rupees.

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Electromagnetic spectrum

January 29th, 2010 by Thomson | No Comments | Filed in Coreelectronics

The information signal should be converted into electronic signals, when free space is the channel. Such signal consists of both electric and magnetic fields. The so-called electromagnetic signals are also referred to as radio frequency (RF) waves.
RF waves oscillate i.e., amplitude of the electric and magnetic fields vary at the specific rate. These oscillations may occur at a very low frequency or at an extremely high frequency. This entire range of frequency is the electromagnetic spectrum. Electromagnetic radiation has an electric field and magnetic field which oscillate in phase perpendicular to each other and to the direction of propagation. Radio frequency band is the frequency or the rate of oscillation within the range of about 3Hz to 300GHz.

electromagnetic spectrum Electromagnetic spectrum

The frequency spectrum extends from subsonic frequencies (a few hertz) to cosmic rays (1022Hz). The International Radio Consultative Committee (CCIR) bands are given below.

Extremely low frequency (ELF) :

ELF range varies from 30Hz to 300Hz and includes ac power signals and low frequency telemetry signals.

Voice frequencies (VFs) :

VF range varies from 300Hz to 3000Hz. Standard telephone channels has 300Hz to 3000Hz bandwidth.

Very low frequency(VLF) :

VLF range varies from 3 KHz to 30 KHz, which includes the upper end of human hearing range. They are used in sub-marine applications.

Low frequency (LF):

LF range varies from 30 KHz to 300 KHz and is used in marine and aeronautical navigation.

Medium frequency(MF):

MF range varies from 300 KHz to 3 MHz and is used for commercial AM broadcasting (535 KHz to 1605 KHz).

High frequency(HF):

HF ranges vary from 3 MHz to 30 MHz and are called short waves. Most of the two-way communications use this range. Amateur radio and citizen band radio also use signals in this range.

Very high frequency (VHF):

VHF range is from 30 MHz to 300 MHz, these are used for mobile, radio, marine, aeronautical communications, commercial FM broadcasting (88 MHz to 108 MHz ) and commercial TV broadcasting (54 MHz to 216 MHz)- channels (2-13).

Ultra high frequency(UHF):

UHF range is from 300 MHz to 3 GHz. It is used for commercial TV broadcasting of channels 14-83, land mobile communication, cellular phones military services, certain radar and navigation systems, microwave and satellite radio systems. Frequencies above 1 GHz are microwaves.

Super high frequency(SHF):

SHF range varies from 3 GHz to 30 GHz and is used in microwave and satellite communication.

Extremely high frequency (EHF):

EHF range varies from 30 GHz to 300 GHz.

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