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It is often said that the transistor is the basic element of amplification, yet it supplies no energy of its own. Exactly what is its role in amplification?

Short Answer

Expert verified
A transistor, despite not supplying any energy, serves as the heart of amplification by controlling the flow of a larger current based on a smaller current. This differential in currents equates to amplification. Thus, a small input signal at the base of the transistor results in an amplified output signal from the collector-emitter pathway due to the transistor’s property of acting as a current switch.

Step by step solution

01

Understanding a Transistor

A transistor is a semiconductor device used to control and manage the flow of electric current. It is made up of two junctions: base-emitter junction (BEJ) and base-collector junction (BCJ) formed by three doped semiconductor regions: Emitter (E), Base (B), and Collector (C)
02

Transistor as a Switch

In its simplest form, a transistor can act like a switch. When a small current (Ib) is applied at the base-emitter junction, it allows a larger current (Ic) to flow from the collector to the emitter. This is because a small change in base-emitter voltage can cause a big change in collector-emitter current.
03

Transistor as an Amplifier

In amplification, the transistor acts similarly to the switch. With the transistor in its active region, a small signal applied to the base is amplified into a much larger signal at the collector. This is how a transistor amplifies a signal: a small variation in input signal at the base, causes a large variation in output signal in terms of current changes. This output has the same frequency as the input, hence it has been amplified.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Semiconductor Device
A transistor is a critical component in electronics and is classified as a semiconductor device. These devices are crafted from materials, like silicon or germanium, that have electrical conductivity between that of a conductor and an insulator.
Semiconductors are special because they can be altered by adding impurities, a process known as doping, to enhance their ability to conduct electricity. This capability allows them to control electrical currents efficiently.
  • Silicon is the most commonly used material for transistors due to its stability and effectiveness at various temperatures.
  • Transistors come in two main types: bipolar junction transistors (BJTs) and field-effect transistors (FETs).
Transistors are foundational elements in both analog and digital circuits, serving as amplifiers and switches that manage the flow of electricity.
Base-Emitter Junction
The base-emitter junction (BEJ) is a vital part of a transistor's operation. It acts like a gate or a valve for the current flow. When a small voltage is applied across the base-emitter junction, it alters the current flowing through the transistor. This junction is forward-biased, meaning it allows current to flow easily from the base to the emitter.
  • The emitter region has a higher doping concentration, which facilitates the emission of charge carriers into the base.
  • The base region is thin and lightly doped, allowing only a small portion of carriers to recombine, which helps in passing the majority to the collector region.
This process is crucial because the small input current at the base controls the larger current flow between the collector and emitter.
Base-Collector Junction
The base-collector junction (BCJ) in a transistor operates primarily as a switch. In normal operation, this junction is reverse-biased, preventing current from flowing directly from the collector to the base.
This reverse-biasing ensures that the charge carriers injected into the base from the emitter are swept into the collector due to the electric field present across this junction.
  • The collector region is generally made larger compared to the emitter and base, which helps it to collect more charge carriers.
  • By maintaining this reverse-bias condition, the junction efficiently controls current flow through the transistor.
This setup is essential for the transistor to function effectively as an amplifier or a switch.
Signal Amplification
Signal amplification is one of the primary functionalities of a transistor. It allows a small input signal at the base to be converted into a larger output at the collector. This amplifying capability hinges on how the transistor modulates current flow.
  • The input signal applied at the base perturbs the base-emitter junction, leading to a corresponding change in the charge flow through the collector.
  • The output signal at the collector maintains the original frequency but with increased amplitude.
This characteristic makes transistors indispensable in electronic circuits, particularly in audio and radio frequency amplifiers. In essence, the transistor acts as a conduit, where a modulated current flow results in signal amplification without adding extra power, maintaining energy balance.

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Most popular questions from this chapter

The magnetic field at the surface of a long wire of radius \(R\) and cairying a current \(I\) is \(\mu_{0} I / 2 \pi R\). How large a curtent could a 0.1 mm diameter niobium wire carry without exceeding its \(0.2 \mathrm{~T}\) critical field?

In Section 10.2. we discussed two-lobed \(p_{\text {re }} p_{\text {s }}\) and \(p_{z}\) states and four-lohed hybrid \(s p^{3}\) states. Another kind of hybrid state that sticks out in just one direction is the sp. formed from a single \(p\) state and an \(s\) state. Consider an urbitrary combination of the \(2 s\) state with the \(2 p_{x}\) state. Let us represent this by \(\cos \tau \psi_{2.0 .0}+\sin T \psi_{2.1 .0}\) (The trig factors ensure norinalization. In carrying out the integral, crow terms integrate to \(0 .\) leaving \(\cos ^{2}+\int\left|\psi_{2,0,0}\right|^{2} d b^{\prime}+\sin ^{2} \tau \int\left|\psi_{21,0}\right|^{2} d V\). which is \(\left.1 .\right)\) (a) Calculate the probability that an electron in such a state would be in the \(+z\) -hemisphere. (Nore: Here. the cross tems do nor integrate to \(0 .\) ) (b) What value of \(r\) leads to the maximum probability. what is the value of the maximum probability, and what is the cotresponding ratio of \(\psi_{2,0.0}\) to \(\phi_{2,1,0} ?\) (c) Using a computer, make a density (shading) plot of the probability density - density versus \(r\) and \(\theta\) for the \(r\) -value found in part (b).

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Based only on the desire to limit minority carriers, why would silicon be preferable to gennanium as a fabric for doped semiconductors?

Carbon (diamond) and silicon have the same covalent crystal structure, yet diamond is transparent while silicon is opaque to visible light, Argue that this should be the case based only on the difference in band gapsroughly \(5 \mathrm{eV}\) for diamond and \(1 \mathrm{eV}\) for silicon.

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