Archive for March, 2010

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.

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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

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