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Analog Circuits unit-1, Lecture notes of Analog Electronics

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K. NIRANJAN KUMAR, Assistant Professor Department Of ECE, VITS, PRODDATUR.
VAAGDEVI INSTITUTE OF TECHNOLOGY & SCIENCE
ANALOG CIRCUITS
UNIT-1 Multistage and Differential Amplifiers
Syllabus:
๏ƒ˜ Introduction โ€“ Recap of Small Signal Amplifiers
๏ƒ˜ Multistage Amplifiers, Cascode amplifier
๏ƒ˜ Darlington pair
๏ƒ˜ the MOS Differential Pair
๏ƒ˜ Small-Signal Operation of the MOS Differential Pair
๏ƒ˜ The BJT Differential Pair
๏ƒ˜ Nonideal Characteristics of the Differential Amplifier.
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VAAGDEVI INSTITUTE OF TECHNOLOGY & SCIENCE

ANALOG CIRCUITS

UNIT- 1 Multistage and Differential Amplifiers

Syllabus:

๏ƒ˜ Introduction โ€“ Recap of Small Signal Amplifiers

๏ƒ˜ Multistage Amplifiers, Cascode amplifier

๏ƒ˜ Darlington pair

๏ƒ˜ the MOS Differential Pair

๏ƒ˜ Small-Signal Operation of the MOS Differential Pair

๏ƒ˜ The BJT Differential Pair

๏ƒ˜ Nonideal Characteristics of the Differential Amplifier.

AMPLIFIER:

A circuit that increases amplitude of given signal is an amplifier. The amplifier is an electronic circuit, which amplifies or increases strength of weak signal.

๏ƒ˜ A small AC signal fed into amplifier is obtained as large AC signal of same frequency. ๏ƒ˜ A amplifier is essential part in radios, TVโ€™s and other communications A linear amplifier magnifies an input signal and produces an output signal whose magnitude is larger and directly proportional to the input signal.

The ac analysis, called a small-signal analysis, can be performed with the dc source set to zero.

Small-Signal Hybrid-ฯ€ Equivalent Circuit of the Bipolar Transistor

All the transistor amplifiers are two port networks having two voltages and two currents. The positive directions of voltages and currents.Out of four variables two can be selected as are independent variables and two are dependent variables.

In h- parameters

๏ƒ˜ (V 1 & I 2 ) โ€“ Dependent Variables ๏ƒ˜ (I 1 & V 2 ) โ€“ Independent Variables

Assuming the transistor as two port network. The iB vs vBE graph the small time varying signal is superimposed on Q-point. The slope of Q-point is constant with units of conductance.

Substitute equation 2 in 1

We can then write the small-signal collector current as ๐’Š๐’„ = ๐’ˆ๐’Ž๐‘ฝ๐’ƒ๐’†

By using above equation we have to draw output port

Combine input port an output port, we will get small signal Hybrid-ฯ€ Equivalent Circuit of the Bipolar Transistor

Fig: A simplified small-signal hybrid- ฯ€ equivalent circuit

Alternative Form of Equivalent Circuit

๐‘–๐ถ = (^) ๐œ• ๐‘–๐œ• ๐‘–๐ถ๐ต |๐‘„โˆ’๐‘๐‘ก. ๐‘–๐ต

๐‘คโ„Ž๐‘’๐‘Ÿ๐‘’ ๐œ• ๐‘– ๐œ• ๐‘–๐ถ๐ต |๐‘„โˆ’๐‘๐‘ก โ‰ก ๐›ฝ

We can then write as ๐’Š๐’„ = ๐œท ๐’Š๐’ƒ

๐’“๐…๐’ˆ๐’Ž = [๐œท๐‘ฝ ๐‘ฐ๐‘ช๐‘ธ๐‘ป ] [๐‘ฐ ๐‘ฝ๐‘ช๐‘ธ๐‘ป ] = ๐œท

Small-Signal Equivalent-Circuit Models:

Fig. MOSFET ๏ƒ˜ The FET behaves as a voltage-controlled current source. ๏ƒ˜ It accepts a signal vgs between gate and source and provides a current gmvgs at the drain terminal. ๏ƒ˜ The input resistance of this controlled source is very high and ideally infinite. ๏ƒ˜ The output resistance looking into the drain also is high, and we have assumed it to be infinite. The DC bias current is ๐ผ๐ท = 12 ๐‘˜๐‘›โ€ฒ ๐‘Š๐ฟ (๐‘‰๐‘”๐‘  โˆ’ ๐‘‰๐‘ก)^2 ๐‘˜๐‘›โ€ฒ^ = ๐œ‡๐‘›๐ถ๐‘‚๐‘‹ VOV = VGS - Vt is the overdrive voltage at which the MOSFET is biased to operate. ๐‘”๐‘š = ๐‘˜๐‘›โ€ฒ ๐‘Š๐ฟ (๐‘‰๐‘”๐‘  โˆ’ ๐‘‰๐‘ก) = ๐‘˜๐‘›โ€ฒ ๐‘Š๐ฟ ๐‘‰๐‘‚๐‘‰

๐‘”๐‘š = (^) ๐‘‰๐‘”๐‘ 2 ๐ผโˆ’๐‘‰๐ท๐‘ก = 2 ๐ผ ๐‘‰๐‘‚๐‘‰๐ท

The small-signal model of the MOSFET

๐’ˆ๐’Ž๐‘ฝ๐…

๐‘… 1 || ๐‘… 2 ||๐‘Ÿ๐œ‹

๐‘‰๐‘‚ = โˆ’๐‘”๐‘š๐‘‰๐œ‹[๐‘Ÿ๐‘œ||๐‘…๐ถ ] ---

And the control voltage ๐‘‰๐œ‹ is found to be

๐‘‰๐œ‹ = (๐‘… 1 ๐‘…||๐‘…^1 ||๐‘… 2 ||๐‘Ÿ^2 ||๐‘Ÿ๐œ‹)+๐‘…๐œ‹ ๐‘ . ๐‘‰๐‘† ---

Substitute eq2 in eq

๐‘‰๐‘‚ = โˆ’๐‘”๐‘š (๐‘… 1 ๐‘…||๐‘…^1 ||๐‘… 2 ||๐‘Ÿ^2 ||๐‘Ÿ๐œ‹)+๐‘…๐œ‹ ๐‘ . ๐‘‰๐‘† [๐‘Ÿ๐‘œ||๐‘…๐ถ ]

๐‘จ๐‘ฝ = ๐‘ฝ ๐‘ฝ๐‘ถ๐‘บ = โˆ’๐’ˆ๐’Ž [๐’“๐’||๐‘น๐‘ช] [ (๐‘น๐‘น๐Ÿ||๐‘น๐Ÿ||๐’“๐…

๐Ÿ||๐‘น๐Ÿ||๐’“๐…)^ + ๐‘น๐’”

]

Assume ๐‘… 1 ||๐‘… 2 ||๐‘Ÿ๐œ‹ = ๐‘…๐ต and ๐‘Ÿ๐‘œ||๐‘…๐ถ = ๐‘…๐ถ

Multistage amplifiers:

๏ƒ˜ In practical applications, the output of a single state amplifier is usually

insufficient, though it is a voltage or power amplifier. Hence they are replaced

by Multistage amplifiers.

๏ƒ˜ A generalized three-stage amplifier is shown in below figure.

Fig. A generalized three-stage amplifier

๏ƒ˜ In Multi-stage amplifiers, the output of first stage is coupled to the input of next

stage using a coupling device. These coupling devices can usually be a

capacitor or a transformer. This process of joining two amplifier stages using a

coupling device can be called as Cascading.

๏ƒ˜ In general, the input impedance of the first stage must be high and the output

impedance of the last must be low.

๏ƒ˜ The overall gain is the product of the individual gains.

Cascode Amplifier :

๏ƒ˜ Cascode amplifier is a type of multistage amplifier. The CE amplifier followed by CB amplifier is called cascode amplifier. The high bandwidth and high gain are major advantages of cascode amplifier. The input is into a common-emitter amplifier (Q 1 ), which drives a common-base amplifier (Q 2 ). The output signal current of Q 1 is the input signal of Q 2.

Fig. Cascode amplifier

F

i g

. Small-signal equivalent circuit of the cascode amplifier

The bias resistance of the amplifier is ๐‘น๐‘ฉ๐Ÿ = ๐‘น๐Ÿ โˆฅ ๐‘น๐Ÿ‘

The input resistance of the amplifier is ๐‘น๐’Š = ๐‘น๐‘ฉ๐Ÿ โˆฅ ๐’“๐…๐Ÿ The out resistance of the amplifier is ๐‘น๐’ = ๐‘น๐‘ช Vฯ€1 = Vs since we are assuming an ideal signal voltage source.

The Voltage gain of the amplifier is

The output voltage is ๐‘‰๐‘œ = โˆ’๐‘”๐‘š2๐‘‰๐œ‹2[๐‘…๐‘ โˆฅ ๐‘น๐‘ณ]^ --- Writing a KCL equation at E 2 , we have ๐‘”๐‘š1๐‘‰๐œ‹1 = ๐‘‰ ๐‘Ÿ๐œ‹2๐œ‹2 + ๐‘”๐‘š2๐‘‰๐œ‹ The control voltage V ฯ€2 (noting that Vฯ€1 = Vs ), we find ๐‘‰๐œ‹2 = ๐‘”๐‘š1๐‘‰๐‘ ๐‘Ÿ๐œ‹2 โˆ’ ๐‘”๐‘š2๐‘‰๐œ‹2 ๐‘Ÿ๐œ‹ ๐‘‰๐œ‹2 + ๐‘”๐‘š2๐‘‰๐œ‹2 ๐‘Ÿ๐œ‹2 = ๐‘”๐‘š1๐‘‰๐‘ ๐‘Ÿ๐œ‹ ๐‘‰๐œ‹2(1 + ๐‘”๐‘š2 ๐‘Ÿ๐œ‹2) = ๐‘”๐‘š1๐‘‰๐‘ ๐‘Ÿ๐œ‹ ๐‘‰๐œ‹2 = (^) (1+๐‘”๐‘”๐‘š1๐‘š2๐‘‰๐‘ ๐‘Ÿ ๐œ‹2๐‘Ÿ๐œ‹2) โˆด ๐›ฝ 2 = ๐‘”๐‘š2 ๐‘Ÿ๐œ‹

๐‘‰๐œ‹2 = ( (^) 1+๐›ฝ๐‘Ÿ๐œ‹2 2 ) ๐‘”๐‘š1๐‘‰๐‘  --- Substitute eq. (3) in eq. (2), we get output voltage as ๐‘‰๐‘œ = โˆ’๐‘”๐‘š1๐‘”๐‘š2 ( (^) 1+๐›ฝ๐‘Ÿ๐œ‹2 2 ) ๐‘”๐‘š1๐‘‰๐‘ [๐‘…๐‘ โˆฅ ๐‘น๐‘ณ] Therefore, the small-signal voltage gain is

๐‘จ๐’—๐’” = ๐‘ฝ ๐‘ฝ๐’๐’” = โˆ’๐’ˆ๐’Ž๐Ÿ๐’ˆ๐’Ž๐Ÿ ( ๐Ÿ+๐œท๐’“๐…๐Ÿ๐Ÿ ) ๐’ˆ๐’Ž๐Ÿ [๐‘น๐’„ โˆฅ ๐‘น๐‘ณ]

We know that ๐‘”๐‘š2 ( (^) 1+๐›ฝ๐‘Ÿ๐œ‹2 2 ) = (^) 1+๐›ฝ๐›ฝ^22 โ‰… 1 The gain of the cascode amplifier is then approximately

๐‘จ๐’—๐’” โ‰… = โˆ’๐’ˆ๐’Ž๐Ÿ [๐‘น๐’„ โˆฅ ๐‘น๐‘ณ]

Which is the same as for a single-stage common-emitter amplifier.

The current gain of the amplifier is ๐‘จ๐‘ฐ๐‘บ = ๐‘ฐ ๐‘ฐ๐‘ถ๐’”

๏ƒ˜ The overall current gain of darrlington pair is multiplication of individual current gains. ๏‚ง If matched transistors then ฮฒ1=ฮฒ2 then ฮฒd=๐›ฝ1^2

๏ƒ˜ Generally darlington pair available in package contain 3 terminals i.e. base ,emitter ,and collector ๏ƒ˜ Darlington pair can be used as emitter follower its equivalent is cascading of two emitter followers.

Fig: A Darlington pair amplifier or configuration The Darlington pair basically consisting of two bipolar transistors with the emitter of one transistor connected to the base of the other, such that the current amplified by the first transistor is amplified further by the second one.

The collectors of both transistors are connected together. It is often packaged as a single transistor. The high current gain and high input impedance are the advantages of Darlington pair. One drawback is doubling of the baseโ€“emitter voltage.

Fig: Small-signal equivalent circuit of Darlington pair ๐‘–๐ธ1 = ๐‘–๐‘1 + ๐›ฝ 1 ๐‘–๐‘1 = ๐‘–๐‘1[1 + ๐›ฝ 1 ] = ๐‘–๐‘2 --- ๐‘–๐ธ2 = ๐‘–๐‘2 + ๐›ฝ 1 ๐‘–๐‘2 = ๐‘–๐‘2[1 + ๐›ฝ 2 ]^ --- Substitute equation 1 in 2 ๐‘–๐ธ2 = ๐‘–๐‘2[1 + ๐›ฝ 2 ] = ๐‘–๐‘1[1 + ๐›ฝ 1 ][1 + ๐›ฝ 2 ]^ --- Current gain

AI = ๐‘– ๐‘–๐ธ2๐‘1 = ๐‘–๐‘1[1+๐›ฝ๐‘–^1 ๐‘1][1+๐›ฝ^2 ]

AI = [1 + ๐›ฝ 1 ][1 + ๐›ฝ 2 ]^ โˆด ๐›ฝ 1 โ‰ซ 1, ๐›ฝ 2 โ‰ซ 1 AI = ๐›ฝ 1 ๐›ฝ 2 โˆด identical transistors ๐›ฝ 1 = ๐›ฝ 2

๐€๐ˆ = ๐œท๐Ÿ๐Ÿ^ = ๐œท๐Ÿ๐Ÿ^ = ๐œท๐‘ซ

Voltage gain

๐ด๐‘‰ = ๐‘‰ ๐‘‰๐‘‚๐‘† = ๐‘–๐ธ2 ๐‘‰๐‘…๐‘†๐ธ = ๐‘–๐‘1[1+๐›ฝ^1 ][1+๐›ฝ ๐‘‰๐‘†^2 ] ๐‘…๐ธ ---

Apply KVL for input loop

๐‘‰๐‘† = ๐‘–๐‘1 ๐‘Ÿ๐œ‹1 + ๐‘–๐‘2 ๐‘Ÿ๐œ‹2 + ๐‘–๐ธ2๐‘…๐ธ ---

Equation 1 convert to equivalent circuit

For calculating output impedance ๐‘‰๐‘† = 0, the above circuit simplified to

๐‘๐‘‚ = (^) ๐‘”^1 ๐‘š ||๐‘…๐ธ โˆดLow resistance || high resistance โ‰… Low resistance โˆด (^) ๐‘”^1 ๐‘š โ‰ช ๐‘…๐ธ

๐’Ž

Differential pair or Amplifier:

๏ƒ˜ The differential-pair or differential-amplifier is the most widely used building block in analog integrated-circuit design. For instance, the input stage of every op-amp is a differential amplifier.

๏ƒ˜ The BJT differential amplifier is the basis of a very-high-speed logic circuit family like emitter- coupled logic (ECL).

๏ƒ˜ Differential Amplifiers is an amplifier in which the output voltage is directly proportional to the difference of input signal. This amplifier, also called a diff-amp There are two input terminals and one output terminal ๐‘ฝ๐’ = ๐‘จ๐‘ฝ๐‘ถ(๐‘ฝ๐Ÿ โˆ’ ๐‘ฝ๐Ÿ) Where A vo is called the open-loop voltage gain.

The differential-mode input voltage ๐‘ฝ๐’… = ๐‘ฝ๐Ÿ โˆ’ ๐‘ฝ๐Ÿ

The common-mode input voltage ๐‘ฝ๐’„๐’Ž = ๐‘ฝ๐Ÿ+๐‘ฝ ๐Ÿ ๐Ÿ

The BJT Differential Pair:

๏‚— The basic BJT differential pair is shown in fig.

Fig. The basic BJT differential pair

Fig: Differential pair with a small differential input signal

๏ƒ˜ From Fig, It can be seen that we are able to steer the entire bias current from one side of the pair to the other with small difference voltages. This current steering property of the differential pair allows it to be used in logic circuits. ๏ƒ˜ Apply a very small differential signal, which will result in one of the transistors conducting a

current of (^) ๐Ÿ๐‘ฐ + ๐šซ๐‘ฐ ; the current in the other transistor will be ๐‘ฐ๐Ÿ โˆ’ ๐šซ๐‘ฐ..

๐‘ฝ๐’ = ๐‘ฝ๐‘ช๐Ÿ โˆ’ ๐‘ฝ๐‘ช๐Ÿ = [๐‘ฝ๐‘ช๐‘ช โˆ’ (๐‘ฐ ๐Ÿ ๐‘ธโˆ’ โˆ†๐‘ฐ) ๐‘น๐‘ช] โˆ’ [๐‘ฝ๐‘ช๐‘ช โˆ’ (๐‘ฐ ๐Ÿ ๐‘ธ+ โˆ†๐‘ฐ) ๐‘น๐‘ช] = ๐Ÿโˆ†๐‘ฐ๐‘น๐‘ช

A voltage difference is created between vC 2 and vC 1 when a differential-mode input voltage is applied.

The magnitude of the small-signal collector current in each transistor is then ( gmvd ) / 2. ๐‘‰๐‘œ = ๐‘‰๐ถ2 โˆ’ ๐‘‰๐ถ ๐‘‰๐‘œ = [๐‘‰๐ถ๐ถ โˆ’ ๐ผ๐ถ2๐‘…๐ถ] โˆ’ [๐‘‰๐ถ๐ถ โˆ’ ๐ผ๐ถ1๐‘…๐ถ] = (๐ผ๐ถ1 โˆ’ ๐ผ๐ถ2)๐‘…๐ถ ๐‘‰๐‘œ = [(๐ผ 2 ๐‘„ + ๐‘”๐‘š 2 ๐‘‰ ๐‘‘) โˆ’ (๐ผ 2 ๐‘„ โˆ’ ๐‘”๐‘š 2 ๐‘‰ ๐‘‘)] ๐‘…๐ถ

Differential mode gain: The ratio of the output signal voltage to the differential-mode input signal is called the differential-mode gain, Ad , which is ๐‘‰๐‘œ = ๐‘”๐‘š๐‘‰๐‘‘๐‘…๐ถ

๐‘ฝ๐’…^ = ๐’ˆ๐’Ž๐‘น๐’„

๐ผ๐‘„ 2 ๐‘‰๐‘‡^ =^

๐ผ๐‘„ 2 ๐‘‰๐‘‡ In many cases output is taken at one collect terminal which is called a one-sided output

๐‘‰๐‘œ = ๐‘”๐‘š๐‘‰ 2 ๐‘‘๐‘…๐ถ

๐‘จ๐’… = ๐’ˆ๐’Ž ๐Ÿ๐‘น ๐‘ช โˆด For Unbalanced output /Single output

Small signal analysis of BJT differential pair