Loading in 5 sec....

Linear Circuit AnalysisPowerPoint Presentation

Linear Circuit Analysis

- By
**danae** - Follow User

- 164 Views
- Uploaded on

Download Presentation
## PowerPoint Slideshow about ' Linear Circuit Analysis' - danae

**An Image/Link below is provided (as is) to download presentation**

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

Presentation Transcript

In an oscilloscope a timing signal called a horizontal sweep acts as a time base, which allows one to view measured input signals as a function of time.

In practice, the linear increase in voltage is approximated by the “linear” part of an exponential response of an RC circuit.

R by the “linear” part of an exponential response of an RC circuit.

+

C

US

_

R

+

L

US

_

First-Order RL and RC Circuits

1. What is a first-order circuit?

A first-order circuit is characterized by a first-order differential equation. It consists of resistors and the equivalent of one energy storage element.

Typical examples of first-order circuits:

(a) First-Order RL circuit

(b) First-Order RC circuit

R by the “linear” part of an exponential response of an RC circuit.

+

C

US

_

+

_

Interconnections of sources, resistors, capacitors, and inductors lead to new and fascinating circuit behavior.

A loop equation leads to

since

First-Order RC circuit

or , equivalently,

This equation is called Constant-coefficient first-order linear differential equation

Apply duality principle,

2. Some mathematical preliminaries by the “linear” part of an exponential response of an RC circuit.

RC circuit first-order differential equation

RL circuit first-order differential equation

The first-order RL and RC circuits have differential equation models of the form

or , equivalently,

valid for t≥t0, where x(t0)=x0 is the initial condition. The term f(t) denotes a forcing function. Usually, f(t) is a linear function of the input excitations to the circuit.

The parameter λdenotes a natural frequency of the circuit.

or by the “linear” part of an exponential response of an RC circuit.

The main purpose of this chapter is to find a solution to the differential equation.

The solution to the equation for t≥t0 has the form

(1) Satisfies the differential equation

(2) Satisfies the correct initial condition, x(t0)=x0

Integrating factor method by the “linear” part of an exponential response of an RC circuit.

First step, multiply both sides of the equation by a so-called integrating factor e－λt.

By the product rule for differentiation,

Integrate both sides of the equation from t0 to t as follows

+ by the “linear” part of an exponential response of an RC circuit.

+

C

R

_

_

+

L

R

_

3. Source-free or zero-input response

A parallel connection of a resistor with an inductor or capacitor without a source.

In these circuits, one assumes the presence of an initial inductor current or initial capacitor voltage.

(a) KCL implies

(b) KVL implies

Both differential equation models have the same general form,

The solution to the equation for by the “linear” part of an exponential response of an RC circuit.t≥t0 has the form

Where τ is a special constant called the time constant of the circuit. The response for t≥t0 of the undriven RL and RC circuit are, respectively, given by

RL circuit

RC circuit

The time constant of the circuit is the time it takes for the source-free circuit response to drop to e－1=0.368 of its initial value.

Linear by the “linear” part of an exponential response of an RC circuit.

Resistive

circuit

No

independent

sources

C

C

L

Linear

Resistive

circuit

No

independent

sources

+

_

+

L

_

For more general circuits, those containing multiple resistors and dependent sources, it is necessary to use the Thevenin equivalent resistance seen by the inductor or capacitor in place of the R.

Thevenin equivalent

Thevenin equivalent

+ by the “linear” part of an exponential response of an RC circuit.

_

Example 1. For the circuit of the figure, find iL(t) and uL(t) for t ≥0 given that iL(0－)=10A and the switch S closes at t=0.4s. Then compute the energy dissipated in the 5Ω resistor over the time interval [0.4, ∞).

R by the “linear” part of an exponential response of an RC circuit.

+

+

+

+

u(t)

R

u(t)

C

US

US

_

_

K

_

_

K

一阶电路的初始条件

稳态（steady state）

代数方程描述

瞬态（transient state）

微分方程描述

（1）问题的提出

US

过渡期为零

换路

过渡状态

过渡状态

US

换路

第一个稳定状态

第二个稳定状态

第三个稳定状态

C by the “linear” part of an exponential response of an RC circuit.

+

_

当

为有限值

（2）电路的初始条件

① t＝0－ 和 t ＝0＋ 的概念

t ＝0－

换路前一瞬间

认为换路在 t ＝0 时刻进行

t ＝0＋

换路后一瞬间

初始条件为t ＝0＋时u、i 及其各阶导数的值

②电容的初始条件

t＝0＋时

电荷守恒

换路瞬间，若电容电流保持为有限值，则电容电压（电荷）换路前后保持不变。

+ by the “linear” part of an exponential response of an RC circuit.

_

L

当

为有限值

③电感的初始条件

t＝0＋时

磁链守恒

换路瞬间，若电感电压保持为有限值，则电感电流（磁链）换路前后保持不变。

④换路定律

反映了能量不能跃变

换路瞬间，若电容电流保持为有限值，

则电容电压（电荷）换路前后保持不变。

换路瞬间，若电感电压保持为有限值，

则电感电流（磁链）换路前后保持不变。

① 画 0－ 等效电路，即换路前电路（稳定状态），求 uC(0－) 和iL(0－)。

电容相当于开路

其中

电感相当于短路

② 由换路定律得 uC(0+) 和 iL(0+)。

③ 画 0+ 等效电路，即换路后的电路。

电容用电压源来替代，大小为 uC(0＋)

其中

电感用电流源来替代，大小为 iL(0＋)。

电压源和电流源的方向均与原来的电压、电流方向一致。

④ 由 0+ 电路求所需各变量的 0+ 值。

单位阶跃函数

延时（delayed）单位阶跃函数

分段常量信号（piecewise-constant signal）

（矩形）脉冲（pulse）

脉冲串（pulse train）

运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。

Example 8.2.运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。 For the circuit of the figure, find iL(t) and uL(t) for t ≥0 given that iL(0－)=10A and the switch S closes at t=0.4s. Then compute the energy dissipated in the 5Ω resistor over the time interval [0.4, ∞).

+

_

Solution

Step 1. With switch S open, compute the response for 0≤t ≤0.4s.

From the continuity property of the inductor current,

Step 2. With switch S closed, compute the response for t≥0.4s.

Step 3.运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。 Write the complete response as a single expression.

Step 4. Plot the complete response.

The 0.4s time constant has a much faster rate of decay than the lengthy 2s time constant.

+运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。

_

Step 5. Compute uL(t).

for 0≤t ≤0.4s,

in particular,

hence,

for t ≥0.4s,

in particular,

Step 6. Compute energy dissipated in the 5Ω resistor over the time interval [0.4, ∞).

+运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。

_

Example 8.3. Find uC(t) for t ≥0 for the circuit of the figure given that uC(0)=9V.

Solution

Step 1. Compute the response for 0≤t ≤1s. By the continuity of the capacitor voltage,

hence,

Step 2. Compute the response for t ≥ 1s.

Step 3. Use step functions to specify the complete response.

Step 4.运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。 Obtain a plot of the response.

Here the part of the response with the 0.3s time constant shows a greater rate of decay than the longer 0.8s time constant.

+运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。

_

Exercise. Suppose that in example 2 the switch moves to the 4.5Ω resistor at t=0.5s instead of 1s. Compute the value uC(t) at t=1.2s.

+运用阶跃函数和延时阶跃函数，分段常量信号可以表示为一系列阶跃信号之和。

+

+

_

_

_

Example 8.4. Find uC(t) for the circuit of the figure, assuming that gm=0.75S and uC(0－)=10V.

Solution

It is straightforward to show that the Thevenin equivalent seen by the capacitor is a negative resistance,

Thevenin equivalent

hence,

Because of the negative resistance, this response grows exponentially, as shown in the figure.

A circuit having a response that increases without bound is said to be unstable.

Negative resistance causes capacitor voltage to increase without bound.

+ exponentially, as shown in the figure.

+

_

_

Exercise. In example 3, let gm=0.125S. Find the equivalent resistance seen by the capacitor and uC(t), t ≥0.

+ exponentially, as shown in the figure.

+

_

_

示例

已知图示电路中的电容原本充有 24V 电压，求K闭合后，电容电压和各支路电流随时间变化的规律。

解：

本题为求解一阶 RC 电路零输入响应问题

则有

又由已知条件

等效电路 t > 0

利用并联分流，得

小结 exponentially, as shown in the figure.

① 一阶电路的零输入响应是由储能元件的初值引起的响应, 都是由初始值衰减为零的指数衰减函数。

RC 电路

RL 电路

② 衰减快慢取决于时间常数 。

RC 电路

RL 电路

R为与动态元件相连的一端口电路的等效电阻。

③ 同一电路中所有响应具有相同的时间常数。

④ 一阶电路的零输入响应和初始值成正比，称为零输入线性。

Linear exponentially, as shown in the figure.

Resistive

circuit

With

independent

sources

C

L

Linear

Resistive

circuit

With

independent

sources

+

+

+

L

_

_

_

+

+

C

_

_

4. DC or step response of first-order circuits

This section takes up the calculation of voltage and current responses when constant voltage or constant current sources are present.

Thevenin equivalent

Thevenin equivalent

+ exponentially, as shown in the figure.

+

L

_

_

+

+

C

_

_

Deriving the differential equation models characterizing each circuit’s voltage and current responses.

By KVL and Ohm’ law,

By KCL and Ohm’ law,

C exponentially, as shown in the figure.

+

+

L

_

_

Exercise. Constant differential equation models for the parallel RL and RC circuits of the figure. Note that these circuits are Norton equivalents of those in the figure. Again choose iL(t) as the response for the RL circuit and uC(t) as the response for the RC circuit.

Answers:

Observe that four differential equations have the same structure:

for RL case

where

for RC case

And the general formula for solving such a differential equation:

where structure:

as long as x(t) is a capacitor

voltage or inductor current, and f(τ)=F is a constant (nonimpulsive) forcing function.

Which is valid for t≥t0. After some interpretation, this formula will serve as a basis for computing the response to RL and RC circuits driven by constant sources.

then structure:

if

for RL case

for RC case

Hence, the solution of the differential equation given constant or dc excitation becomes

for RL case

for RC case

+ structure:

+

_

_

Example 8.5. For the circuit of the figure, suppose a 10V unit step excitation is applied at t=1 when it is found that the inductor current is iL(1－)=1A. The 10V excitation is represented mathematically as uin(t)=10u(t－1)V for t≥1. Find iL(t) and uL(t) for t≥1.

Solution

Step 1. Determine the circuit’s differential equation model.

where the time constant

Step 2. Determine the form of the response.

+ structure:

+

_

_

Step 3. Compute iL(∞) and set forth the final expression for iL(t).

replace the inductor by a short circuit,

and since

It follows that,

Step 4. Plot iL(t).

Exercise. structure: Verify that in example 4, uL(t) can be obtained without differentiation by

+

+

Specifically, we need only compute , , and the time constant or .

_

_

Step 5. Compute uL(t).

Exercise. In example 4, suppose R is changed to 4Ω. Find iL(t) at t=2s.

+ structure:

+

_

_

Example 8.6. The source in the circuit of the figure furnishes a 12V excitation for t<0 and a 24V excitation for t≥0, denoted by uin(t)=12u(－t)+24u(t)V. The switch in the circuit closes at t=10s. First determine the value of the capacitor voltage at t=0－, which by continuity equals uC(0+). Next determine uC(t) for all t≥0.

Solution

Step 1. Compute initial capacitor voltage

Step 2. Obtain uC(t) for 0≤t ≤ 10s.

+ structure:

+

+

+

_

_

_

_

Step 3. Compute the initial condition for the interval t>10.

Step 4. Find uC(t) for t>10.

Thevenin equivalent

Step 5. Set forth the complete response using step functions.

Step 6. structure: Plot uC(t).

Exercise. Suppose the switch in example 5 opens again at t=20s. Find uC(t) at t=25s.

+ structure:

+

_

_

示例

t = 0 时 , 开关K闭合，已知 uC(0－) = 0V，求（1）电容电压和电流；（2）uC＝80V 时的充电时间 t。

（1） RC 电路零状态响应问题

解：

（2）设经过 t秒，uC＝80V

全响应的两种分解方式 structure:

稳态分量

US

① 根据电路的两种工作状态

全响应

U0

稳态分量

暂态分量

全响应

暂态分量

U0－US

物理概念清晰

②根据激励与响应的因果关系

US

零状态响应

全响应

U0

零输入响应

零状态响应

全响应

零输入响应

便于叠加计算

+ structure:

+

+

_

_

_

例2

t = 0 时 , 开关K闭合，求 t > 0 后的 iC，uC 以及电流源两端的电压 u，已知 uC(0+) = 1V。

解：

RC电路全响应问题

稳态分量

全响应

故

is . structure:

5. Superposition and linearity

Provided one properly accounts for initial conditions, superposition still apply when capacitors and inductors are added to the circuit.

for a capacitor

suppose

and

By the same arguments, the current due to the input excitation

One the other hand, suppose structure:

and

Thus linearity and, hence, superposition hold.

Arguments analogous to the preceding imply that a relaxed inductor satisfies a linear relationship, and thus superposition is valid, whether the inductor is excited by currents or by voltages.

For a general linear circuit, one can view each initial condition as being set up by an input which shuts off the moment the initial condition is established.

This mean that when using superposition on a circuit, one first looks at the effect of each independent source on a circuit having no initial conditions.

Then one sets all independent sources to zero and computes the response due to each initial condition with all other initial conditions set to zero.

The sum of all the responses to each of the independent sources plus the individual initial condition responses yields the complete circuit response, by the principle of superposition.

_ condition as being set up by an input which shuts off the moment the initial condition is established.

+

+

_

Example 8.8. The linear circuit of the figure has two source excitations applied at t=0, as indicated by the presence of the step functions. The initial condition on the inductor current is iL(0－)=－1A. Determine the response iL(t) for t≥0 using superposition.

Solution

Step 1. Compute the part of the circuit response due only to the initial condition, with all independent sources set to zero.

_ condition as being set up by an input which shuts off the moment the initial condition is established.

+

+

_

Step 2. Determine the response due only to US=10u(t)V.

Step 3. Compute the response due only to the current source IS=2u(t)A.

Step 4. condition as being set up by an input which shuts off the moment the initial condition is established. Apply the principle of superposition.

due to source US

due to source IS

due to initial condition

The question still remains as to why the superposition principle holds an advantage over the Thevenin equivalent method.

Question 1. What is the new response if the initial condition is changed to iL(0－)=5A?

Question 2. What is the new response if the voltage source US is changed to 5u(t)V, with all other parameters held constant at their original values?

Question 3. What is the new response if the initial condition is changed to 5A, the voltage source US is changed to 5u(t)V, and the current source IS is changed to 8u(t)A?

This allows one to explore easily a circuit’s behavior over a wide range of excitations and initial conditions.

6. Response classifications principle holds an advantage over the Thevenin equivalent method.

Zero-input response The zero-input response of a circuit is the response to the initial conditions when the input is set to zero.

Zero-state response The zero-state response of a circuit is the response to a specified input signal or set of input signals given that the initial conditions are all set to zero.

Complete response By linearity, the sum of the zero-input and zero-state responses is the complete response of the circuit.

Natural response The natural response is that portion of the complete response that has the same exponents as the zero-input response.

Forced response The forced response is that portion of the complete response that has the same exponents as the input excitation.

7. Further points of analysis and theory principle holds an advantage over the Thevenin equivalent method.

Not only a capacitor voltage or an inductor current, it turns that any voltage or current in an RC or RL first-order linear circuit with constant input has the form

by linearity, any voltage or current in the circuit has the form

and

which implies that

+ principle holds an advantage over the Thevenin equivalent method.

+

+

+

_

_

_

_

Example 8.9. For the circuit of the figure, let uin(t)=－18u(－t )+9u(t)V. Find iin(t) for t>0.

Solution

Step 1. Compute iin(0+).

0+ circuit

Step 2. Computeτand iin(∞).

+ principle holds an advantage over the Thevenin equivalent method.

+

_

_

Step 3.Set forth the complete response iin(t).

Exercise. In example 7, find iC(0－), iC(0+), and iC(t) for t>0.

+ principle holds an advantage over the Thevenin equivalent method.

_

+

+

+

_

_

_

例1

t = 0 时开关闭合，求 t > 0 后 iL，i1 和 i2。

解法1：

+ principle holds an advantage over the Thevenin equivalent method.

_

+

_

例1

t = 0 时开关闭合，求 t > 0 后 iL，i1 和 i2。

解法2：

+ principle holds an advantage over the Thevenin equivalent method.

+

_

_

+

_

_

_

+

+

例2

t = 0 时开关由1→2，求换路后的uC(t) 。

解：

戴维宁等效

+ principle holds an advantage over the Thevenin equivalent method.

_

例3

t = 0 时 , 开关闭合，求换路后的i(t) 。

解：

+ principle holds an advantage over the Thevenin equivalent method.

_

例4

已知：电感无初始储能，t = 0 时闭合K1，t =0.2s时闭合K2 ，

求两次换路后的电感电流。

解：

Download Presentation

Connecting to Server..