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Introduction

image-20230314230251154

Kirchhoff’s Current & Voltage Law

nn-node bb-branch circuit:

  • n1n-1 independent KCL Eqs.
  • bn+1b-n+1 independent KVL Eqs.

Nodal Analysis

Goal: Finding Node Voltages.

Assumption: Circuits Having no voltage source.

image-20230314230817493

  1. Selecting reference node and assigning voltages to remaining nodes. 非参考节点的个数等于独立方程的个数。
    1. Common ground
    2. Ground
    3. Chassis ground (基座)
  2. Applying KCL to each nonreference nodes and expressing IbranchI_{\mathrm{branch}} in terms of VnodeV_{\mathrm{node}}.
    1. Element Voltage
    2. PSC: i=vhvlRi = \frac{v_{h}-v_{l}}{R}. 通过电阻的电流总是从高电位向低电位流动。认为电流方向的起始点为高电位,电流方向的终止点为低电位。
    3. Solve Eqs. by Substitution method, Elimination method, Cramer’s rule, Matrix inversion.
  3. Solving simultaneous Eqs. to obtain unknown voltages.

image-20230302214322387

{10=i1+i2i1=i3+4ixi2+4ix=ixi2=v1v32i3=v1v23\left\{ \begin{matrix}10=i_1+i_2\\i_1=i_3+4i_x\\i_2+4i_x=i_x\\i_2=\frac{v_1-v_3}{2}\\i_3=\frac{v_1-v_2}{3}\end{matrix}\right.

Nodal Analysis with Voltage Sources

Case 1

Voltage source connected between reference node and non reference node

Case 2

Independent or dependent voltage source connected between two nonreference nodes.

image-20230315153009402

Forming a supernode. iin=iouti_\mathrm{in}=i_{\mathrm{out}}

Introduced because the current through voltage source is unknown. “缩边、缩点”

image-20230302215124433

image-20230302220413219

image-20230315154036755

i1=i2+i3+i4i1=(14v)/4i2=v/3i3=i=(v+6)/2i4=(v+6)/6i_1=i_2+i_3+i_4\\ i_1=(14-v)/4\\ i_2=v/3\\ i_3=i=(v+6)/2\\ i_4=(v+6)/6

v=2/5V=400mV,i=2.8Av=-2/5 V=-400mV,i=2.8A.

image-20230315154735046

Mesh Analysis

  • A loop: a closed path with no node passed more than once.
  • A mesh: a loop that does not contain any other loops within it.

Planar circuit.

  1. Assign mesh currents to nn meshes.
  2. Applying KVL to each mesh and expressing voltages in terms of mesh currents. (Nodal: voltage $\to $ current)
  3. Solving simultaneous Eqs to obtain unknown currents.

image-20230315155132893

image-20230315155608747

image-20230315155827106

1510=15i110i210=20i210i115-10=15i_1-10i_2 \quad 10=20i_2-10i_1

电流方向符合 ASC,等号另一边就是正的。

Mesh Analysis with Current Sources

  1. Only in one mesh.

  2. Between two meshes. \Rightarrow Supermesh. Voltage across current source is not known. Formed by excluding current source and any elements connected in series with it.

    image-20230315160409433

Current Sources have corresponding voltages.

Assume additional voltages.

image-20230306101638674

image-20230306102833130

image-20230306102854169

Nodal Analyses by Inspection

取进入节点为正值

image-20230315161213673

Gkk:G_{k k}: \quad Sum of conductances directly connected to node kk
Gkj=GjkG_{k j}=G_{j k} : Negative of sum of conductances directly connecting nodes kk and j,kjj, k \neq j.
vk:v_k: \quad Unknown voltage at node kk
iki_k : \quad Sum of all independent current sources directly connected to node kk, with currents entering node treated as positive

This is valid for circuits with only independent current sources and linear resistors.

image-20230306110423671

image-20230306110502841

image-20230306110525778

image-20230306111257646

image-20230306111336385

image-20230306111353973

Mesh Analyses by inspection

和网孔分析法一样,取ASC方向的电源为正值。

image-20230315161331754

image-20230306111710439

image-20230306112233267

![image-20230306112254539](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230306112254539.png)

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Notes

Dependent Sources \Rightarrow not symmetric.

Both voltage sources and current sources. Form KCL/KVL.

image-20230306113938732

Examples

image-20230308081120588

100=10i1+40i2120+80i3i3i2=2i2100=10i_1+40i_2-120+80i_3\\ i_3-i_2=2i_2

image-20230308081634509

RΔ=AB+BC+ACAR_{\Delta}=\frac{AB+BC+AC}{A}

YΔY-\Delta Transformation.


image-20230311192112078

image-20230311192944592

i3=i2+α3i3i2=i1+α2i2i1+i=α1i1α1i1+α2i2+α3i3=i3+ivsiR1=vi_3=i_2+\alpha_3i_3\\ i_2=i_1+\alpha_2i_2\\ i_1+i=\alpha_1i_1\\ \alpha_1i_1+\alpha_2i_2+\alpha_3i_3=i_3+i\\ v_s-iR_1=v

Problems

Chapter 3, Problem 40.

![image-20230401200731506](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401200731506.png)

Assume all currents are in mA\mathrm{mA} and apply mesh analysis for mesh 1.

30=12i16i24i315=6i13i22i330=12i_1-6i_2-4i_3 \Rightarrow 15=6i_1-3i_2-2i_3

for mesh 2,

14i26i12i3=03i1+7i2i3=014i_2-6i_1-2i_3=0\Rightarrow-3i_1+7i_2-i_3=0

for mesh 3,

10i34i12i2=05i32i1i2=010i_3-4i_1-2i_2=0 \Rightarrow 5i_3-2i_1-i_2=0

Chapter 3, Problem 41.

Apply mesh analysis to find ii in Fig. 3.87.

![image-20230401201050881](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401201050881.png)

For loop 1,

6=12i12i23=6i1i26=12i_1-2i_2\Rightarrow 3=6i_1-i_2

For loop 2,

7i2+82i1i3=07i_2+8-2i_1-i_3=0

For loop 3,

8+6+6i3i2=02=i2+6i3-8+6+6i_3-i_2=0\Rightarrow 2=-i_2+6i_3

Chapter 3, Problem 44.

Using Super Mesh

![image-20230401201603445](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401201603445.png)

Loop 1 and 2 form a supermesh. For the supermesh. (We assume i1i_1 and i2i_2, the total number of variables assumed in supermesh is equal to ordinary mesh analysis, however, we consider the corresponding current with respect to each branch)

6i1+4i25i3+12=06i_1+4i_2-5i_3+12=0

For loop 3,

i14i2+7i3+6=0-i_1-4i_2+7i_3+6=0

i2=3+i1i_2=3+i_1

Chapter 3, Solution 45.

![image-20230401202238720](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401202238720.png)

Chapter 3, Solution 46.

![image-20230401202407398](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401202407398.png)

Chapter 3, Problem 51.

![image-20230401202647493](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401202647493.png)

We can only tell that i1i_1 equals to 5A because the voltage across the current source is unknown.

Chapter 3, Problem 60.

![image-20230401203104742](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401203104742.png)

io=v11i_o=\frac{v_1}{1}

At node 1,

v11+0.5v11=10v14\frac{v_1}{1}+\frac{0.5v_1}{1}=\frac{10-v_1}{4}

At node 2,

0.5v11+10v28=v22\frac{0.5v_1}{1}+\frac{10-v_2}{8}=\frac{v_2}{2}

Chapter 3, Problem 62.

Find the mesh currents i1,i2i_1,i_2 and i3i_3 in the network of Fig. 3.106.

![image-20230401205313101](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401205313101.png)

Supermesh

Chapter 3, Problem 63.

![image-20230402210309356](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230402210309356.png)

![image-20230402210541084](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230402210541084.png)

Chapter 3, Problem 64.

![image-20230401205557414](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401205557414.png)

Using Super Mesh. Excluding current sources.

![image-20230401205658037](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230401205658037.png)

We don’t have to assume ^ this mesh current, because there are no passive elements on this mesh.

For the super mesh,

50i1+10i1+40i31004i010i2=050i_1+10i_1+40i_3-100-4i_0-10i_2=0

For the smaller mesh,

20i2+4i010i1=020i_2+4i_0-10i_1=0

Now we have 2 equations for 4 unknowns, so we need 2 extra equations.

For the first equation, use KCL,

i1=i2+i0i_1=i_2+i_0

For the second equation, see B as a node.

2+i3=0.2v0+i1vo=2i22+i_3=0.2v_0+i_1\quad v_o=2i_2

Chapter 3, Problem 67

![image-20230402201334343](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230402201334343.png)

![image-20230402201846137](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230402201846137.png)

代回原式即可解。

Chapter 3, Problem 73.

![image-20230402202318914](C:\Users\Steven Meng\AppData\Roaming\Typora\typora-user-images\image-20230402202318914.png)

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