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Operational amplifier tester. Encyclopedia of radio electronics and electrical engineering

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Encyclopedia of radio electronics and electrical engineering / Measuring technology

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You can check the performance of the operational amplifier by turning it on as a simple square-wave generator. The figure shows a diagram that allows you to implement this method in practice.

Operational amplifier tester

When button S1 is pressed, the input of the op-amp maintains a reference voltage obtained from the output voltage through the voltage divider R2/R3. The current through resistor R1 is used to charge capacitor C1 until the voltage level at the inverting input reaches the reference voltage level. The op amp now acts as a comparator, its output level changing state, thus producing a reference voltage of opposite polarity. The charge current for C1 will then flow in the opposite direction until the new reference voltage is reached and the whole cycle is repeated.

When the output is high, transistor T1 will be turned on and LED D1 will be lit. Conversely, when the output is low, transistor T2 is on and LED D2 is lit.

The transistors are connected so that other op amps with the same pinout but less output current than the 741 IC can be tested.

The tester requires positive and negative power supplies to operate. Satisfactory operation is ensured by the use of two 9-volt batteries.

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Random news from the Archive

A new type of strange quasicrystals 17.01.2019

Physicists and chemists at Brown University have for the first time created a self-assembling quasi-crystal lattice, consisting of quantum dots of a strictly defined shape. Similar quasicrystalline lattices have already been described mathematically and calculated in the course of complex computer simulations more than once, but no one has previously been able to demonstrate their creation, as they say, live.

We remind our readers that crystals are structures consisting of homogeneous components and possessing symmetry in one or more spatial coordinates. In other words, if we take any section of the crystal and shift it to a certain distance along the axis of symmetry, then the structure of the shifted section will completely coincide with the structure of the "unshifted" section. Quasicrystals do not have such a symmetry, their components are arranged in space in an ordered manner, but the structure of a quasicrystal does not repeat itself.

The mathematical description of quasicrystals is quite easy to create, but, as previously thought, the creation of aperiodic crystal structures in reality is impossible. Some time ago, scientists have already observed signs of the existence of quasi-crystals in aluminum alloys that have gone through a complex process of synthesis and heat treatment, and this fact was the first confirmation of the possibility of their existence. At present, the fact of the existence of quasicrystals is considered already proven, and they are considered a new potentially useful type of material.

So let's get back to the material created at Brown University. Interestingly, scientists initially did not even think about quasicrystals, their task was to find new methods for building macrostructures from nanosized components. One of the types of components was a pyramidal quantum dot, a tetrahedral particle, about one nanometer in size. Preliminary calculations have shown that such a shape will allow "packing" in a certain volume of space a greater number of such particles than particles of a traditional spherical shape.

Tetrahedral particles had one more feature, they behaved and interacted with neighboring particles in different ways, depending on their current spatial orientation. And as a result of this, after a while, all the particles spontaneously ordered, creating a complex structure, which is known as a quasi-transparent superlattice.

Electron microscope studies of this structure have shown that the particles form decagonal patterns, united by a symmetry of a kind never found in traditional crystals. The only exception is the boundaries of the material, where, in order to optimally fill the space, the particles are combined into patterns with fewer corners.

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