Showing posts with label meter. Show all posts
Showing posts with label meter. Show all posts

Monday, October 20, 2014

Check Inductors With This Simple Q Meter


While LCR meters are readily available at reasonable cost, they do not measure the Q of an inductor. This circuit enables you to measure the Q of inductors with the aid of an RF signal generator. A capacitor is connected in parallel with the inductor to form a tuned circuit. By varying the frequency, you can measure the resonance frequency of the tuned circuit and its -3dB bandwidth. The Q is then the resonance frequency divided by the -3dB bandwidth. Transistor Q1 is an emitter follower acting as input buffer to drive RF transformer T1. The secondary winding of T1 then drives the parallel tuned circuit formed by the inductor under test (Lx), T1’s secondary and tuning capacitor VC.

The tuned circuit so formed is buffered by JFET Q2 and transistor Q3 which form a cascode stage with about 3dB of gain. The JFET provides a high impedance so that the loading of the tuned circuit is minimal (note: an MPF102 can be substituted if you cannot obtain a 2N5485). The RF output from Q2s collector can be monitored by an oscilloscope to easily find the point of resonance and read the frequency. Alternatively, the RF output can be read by an external frequency meter. Diodes D1 & D2 and the 5.6nF capacitors form a voltage doubler rectifier to drive a 100µA DC meter so that the resonance can be found (in the absence of an oscilloscope).

Check inductors with this simple Q meter
Trimpot VR1 provides a sensitivity adjustment for the meter. Transformer T1 is wound on a 12mm diameter ferrite toroid core. The primary winding consists of 50 turns of 0.2mm diameter enamelled copper wire, while the secondary is a single turn consisting of a strip of brass 0.5mm thick and 2.5mm wide bent into a horseshoe shape and threaded through the centre of the toroid. VC is a small AM tuning capacitor with both gangs connected in parallel.

To measure Q, the output of the RF signal generator should be around 0.5V peak. Adjust the frequency until the meters reading peaks, then adjust VR1 so that the meter reads full scale (100µA). Read the resonance frequency F0 from the frequency scale of the signal generator or better still, the reading on a frequency meter.

Next, increase the signal frequency until the meter reads 70µA and note this frequency as F2. That done, reduce the frequency on the signal generator below the resonance frequency until the meter again reads 70µA and note this frequency as F1. The Q can now be calculated as:

Q = F0/(F2 - F1)

While using a variable tuning capacitor will enable a wider range of inductors to be tested, the main advantage is estimating the distributed capacitance of the inductor as well. To do this, you have to calibrate the tuning scale with a capacitance meter, by measuring the capacitance across the tuning capacitor with no inductor connected. This is done with the unit switched off. Marking off increments of 20pF should be sufficient.

Set the tuning capacitor to say ¼ of its maximum value and note this value as C1. Adjust the RF signal generator frequency so that the inductor under test is at resonance and note this frequency as F0. Now set the RF generator frequency to half F0, adjust the tuning capacitor until resonance and note this capacitance as C2. The distributed capacitance of the inductor is (C2 - 4C1)/3.
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Wednesday, February 26, 2014

Minimalist Dip Meter

In days gone by a radio amateur always had a dip meter close to hand in his ‘shack’. Now that people can afford oscilloscopes, the poor old dip meter has lost its importance and is  frequently no longer to be seen. Actually this is a shame because many tasks are much easier to carry out with a dip meter. Anyone who’s interested (perhaps the second time around) can easily build one rapidly with this very simple but adequate circuit. The interesting question is namely what do you actually need from a dip meter? 

Minimalist Dip Meter-Circuit Diagram Minimalist Dip Meter Circuit Diagram
  • A visual display of the dip? Nope, the ‘scope can handle that task.
  • A large frequency scale? Not necessary, as you can connect a frequency counter for this.
  • A selection of coils? We don’t need these because we can use a jumper to change range (no coils to lose any more!).
The sensor coil L1 has ten turns and is wound  using an AA-size battery as a former. This coil will allow us to over the range from 6 MHz to 30 MHz. With jumper JP1 open an additional fixed inductance of 10 μH comes into circuit. The frequency measurement range is then from 2.5 MHz to 10 MHz. The switch may be replaced by a jumper. 

To take measurements you hold a resonant circuit close to the sensor coil. Tune the rotary capacitor C1 slowly to and fro in order to find the resonant frequency, at which the oscillator amplitude decreases somewhat. The frequency can then be read directly off the oscilloscope.
To obtain a very accurate measurement you can additionally connect your frequency counter to the second output.


http://www.ecircuitslab.com/2012/05/minimalist-dip-meter.html
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Friday, January 31, 2014

Water Tank Level Meter Sensor

The water-tank level meter de-scribed here is very simple and useful for monitoring the water level in an overhead tank (OHT). The water level at 30cm intervals is monitored and continuously indicated by LEDs ar-ranged in a meter-format. When all the LEDs are ‘off’, it indicates that the OHT is empty. When the water level reaches the top limit, the whole LED-meter begins to flash. The height at which the level-sensing electrodes are fitted is adjustable. Thus, the minimum and maximum level settings may be varied as desired. The range of the meter can also be enlarged to cater to any level. No special or critical components are used. CMOS ICs are used to limit the idle current to a minimum level.
 
Even when all the LEDs are ‘on’, i.e. water reaches the top level, the demand on the power supply is reasonably low. Further, the extremely high input resistance of the Schmitt inverter gates reduces the input current and thus minimises the erosion of electrodes. The princi-pal part of the device is its water-level sensor assembly. By using easily available material, it can be fabricated to meet one’s own specific requirements. The common ground reference electrode ‘X’ is an aluminium conduit of 15mm outer diameter and 3-metre length, to cater to a 3-metre deep overhead tank. Insulating spacer rings ‘Y’ (10mm length, 15mm dia.) are fabricated from electrical wiring conduits of 15mm inner diameter.
 
These are pushed tightly over the aluminum conduit at preferred places, say 30cm apart. If the pieces are too tight, they can be heated in boiling water for softening and then pushed over ‘X’. The sensor electrodes ‘Z’ are made out of copper or brass strips (6mm wide and 1mm thick) which are shaped into rings that can tightly slip over the ‘Y’ pieces. The ends of these strips are folded firmly and formed into solder tags S1 to S10 and SG. The wall-mounting brackets, made of aluminium die-cast, are screwed directly on ‘X’ at two suitable places.
 
Water-Tank Level Meter cir 
The sensor cable ‘WC’ wires are soldered to solder tags, and some epoxy cement is applied around the joints and tags to avoid corrosion by water. The common ground reference wire ‘SG’ is taken from tag ‘T’. The cable’s individual wires from S1 to S10 and SG are cut and matched in length for a neat layout. The other ends of the cable are connected to the PCB terminal points S1 to S10 and SG respectively. No separate ground is needed. The electronics portion is simple and straightforward. A long piece of vero board can hold all the parts including the power supply section.
 
For easy installation, the LEDs can be set at the track side of the board, in a single line, so that they may be pushed through the cutouts in the front panel of the enclosure from inside. The water level at 30cm intervals is monitored by corresponding sensors, causing the input  to the concerned inverters (normally pulled  ‘high’ via resistors R1 through R10) to go ‘low’, as soon as water reaches the respective sensors On initial switching  ‘on’ of the power supply, when the tank is empty, all the electrodes are open. As a result, all the inverter inputs are ‘high’ (via the pull-up resistors R1 to R10) and their outputs are all  ‘low’. Thus, all the LEDs are  ‘off ’. As soon as the water starts filling the tank, the rising water level grounds the first sensor.
 
The logic 1 output of first inverter gate N1 causes conduction of transistor T2 to extend ground to one side of resistors R14 through R23 via emitter collector path of transistor T2. The LED D1 is thus lit up. Similarly, other LEDs turn  ‘on’ successively as the water level rises. As soon as the water in OHT reaches the top level, the output of gate N10 goes to logic 1 and causes flashing-type LED D11 to start flashing. At the same time, transistor T1 conducts and cuts off alternately, in synchronism with LED D11’s flash rate, to ground the base of transistor T2 during conduction of transistor T1. As a result, transistor T2 also starts cutting ‘off’ during conduction of transistor T1, to make the LED meter (comprising LEDs D1 through D10) flash and thus warn that the water has reached the top level.
 
When the water level goes down, the reverse happens and each LED is turned ‘off’ successively. The novel feature of this circuit is that whenever the water level is below the first sensor, all the LEDs are ‘off’ and the quiescent current is very low. Thus, a power ‘on’/‘off’ switch is not so essential. Even when the LED-meter is fully on, the cur-rent drawn from the power supply is not more than 120 mA. A heat-sink may, how-ever, be used for transistor T2, if the tank is expected to remain full most of the time. A power supply unit providing unregulated 6V DC to 15V DC at 300mA current is adequate.
 
Caution. A point to be noted is that water  tends to stick to the narrow space at the sensor-spacer junction and can cause a false reading on the LED-meter. This can be avoided if the spacers are made wider than 10 mm.
Author : M.K. Chandra MouleeswAran - Copyright : EFY
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Sunday, January 12, 2014

Measure your stress level – Tension meter

If you, like so many other people in this day and age, arrive home from work stressed out and with the problems of the day still lingering,this simple little instrument will go a long way to relieving nervous tension.
Of the various types of feedback devices, probably the best approach for the amateur experimenter is the Galvanograph, better known as the Galvanic Skin Response Monitor. The instrument described here relies for its operation on changes in skin resistance in sympathy with changes in emotional state. An increase in tension level reduces skin resistance and, conversely, a decrease in tension is accompanied by an increase in skin resistance.
The correlation between emotional stress and skin resistance is still not fully understood. What is known, though, is that minute changes in the permeability of the skin produce corresponding voltage variations across two electrode pads attached to two fingers on the same hand.

Measure tension meter


Tension Monitor meter circuit

These signal fluctuations are amplified and fed to an oscillator to produce an audible tone. A decrease in pitch therefore signifies a decrease in tension, and vice-versa. A visual indicator in the form of a panel meter also aids the user in monitoring tension levels. The monitor is quite sensitive to fluctuations. During use, a sudden moment of stress, even a deep sigh, will increase the pitch and cause a shift of the meter needle. Circuit Details In the circuit diagram of Fig.1, IC1 is configured as an astable multivibrator to drive an 8-ohm miniature speaker LS1 via capacitor C3, resistor R6 and volume control potentiometer VR2. The latter allows users to set a desired level and avoid it becoming a distraction.
Whereas the trigger input of IC1 is normally connected to the positive rail via a resistor in a conventional 555 oscillator, here it is connected via resistor R4 to the emitter of transistor TR1. The base of TR1 is connected between one electrode pad and the voltage divider formed by potentiometer VR1 and resistor R1. It will be seen that with the pads fitted to the fingers, the tone level will be dependent on the setting of VR1 and skin resistance. Resistor R2 in the transistor base is necessary should the pads be accidentally touched together. A 1mA meter is fitted in the collector line, along with R3, as a visual indicator. Although not essential or intended to measure current levels, it does help to emphasize fluctuations in emotional level.
The design of the pads is not critical. For the prototype, stripboard was used. The tracks were wired together at one end and connected to a 30cm length of twin lighting flex. The pads were then glued to Velcro straps. When the unit is first switched on, a highpitched tone should be heard, rapidly diminishing and ceasing. Turn the Sensitivity control VR1 to the minimum setting. Attach the electrodes to the fleshy pads of the first two fingers on the less-dominant hand with the Velcro straps, firmly but not tight. Rest the hand comfortably and keep it reasonably still, allowing half a minute for the pads to “bond”. Normally, at the minimum setting, the oscillator will hardly tick over, unless the user is in a high state of anxiety. Keep in mind that any form of stimulant, and that includes tea, coffee, alcohol and cigarettes, will reduce one’s capacity to relax. Rotate the control until a medium pitched tone is obtained and apply your relaxation technique. The monitor does not teach any method of meditation or relaxation; it only monitors the effectiveness of the technique applied. The tone should slowly diminish, with fluctuations as unconscious thoughts flit across the mind.When the sound ceases altogether, repeat the above procedure by increasing VR1. Twenty minutes is considered by therapists to be an adequate relaxation session.
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Sunday, November 17, 2013

LED Audio Level Meter Circuit

This circuit uses two quad op-amps to form an eight LED audio level meter. The op-amp used in this particular circuit is the LM324. It is a popular IC and should be available from many parts stores.

LED audio level meter
LED audio level meter schematic
The 1K resistors in the circuit are essential so that the LEDs turn on at different audio levels. There is no reason why you cant change these resistors, although anything above 5K may cause some of the LEDs to never switch on. This circuit is easily expandable with more op-amps, and is not limited to use with the LM324. Pretty much any op-amp will work as long as you look up the pinouts and make sure everything is properly connected.

The 33K resistor on the schematic is to keep the signal input to the circuit at a low level. It is unlikely you will find a 33K resistor, so the closest you can get should do. The value of this resistor may need to be changed, so it is best you breadboard this circuit before actually constructing it on PCB. The circuit in its current form will accept line level inputs from sources such as the aux out on a Hi-Fi, all though could be easily modified to accept speaker inputs.

The audio + is connected to the main positive rail, while the audio - is used for signal input. The 50k pot can be used to vary the sensitivity of the circuit.
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