2.1 ohm's law 2.3 resistors combinations 2.2 kirchhoff's laws chapter 2 basic laws...
TRANSCRIPT
2.1 Ohm's Law
2.3 Resistors Combinations
2.2 Kirchhoff's Laws
Chapter 2 Basic Laws 基本定律
2.1 Ohm’s Law 欧姆定律
iv RR0
+ -v
i R
Ohm's law states that the voltage Ohm's law states that the voltage vv across a resistor across a resistor is directly proportional to the current is directly proportional to the current i i flowing flowing
through the resistor.through the resistor.
(欧姆)
resistorresistor
resistanceresistance
电阻(名称)
电阻值
Pay attention:
A short circuit is a circuit element with resistance approaching zero.
0
0
0
i
Riv
R
A short circuit (R = 0)A short circuit (R = 0)
RR=0=0
ii
v=0Network
Short Circuit: 短路
An open circuit is a circuit element with resistance approaching infinity (无限大) .
0
0
vR
vi
R
An open circuit (R=An open circuit (R=))
RR==
ii=0=0
vvNetwork
Open Circuit : 开路
v
i0
Slope=R
v
i0
Slope=R
The v~i characteristic (电压 ~ 电流特性) of:
(a) a linear resistor, (b) a nonlinear resistor.
iv R
NOTE :
1. The power is nonlinear function of either current or voltage.
v
i
RG
1
Conductance (G) (电导)
The power can be expressed in terms of R.
02
2 R
vRivip
S( 西门子)
(姆欧)
2. A resistor always absorbs power (吸收功率) from the circuit. A resistor is a passive element.
1 nbl
Ⅰ. Nodes, Branches and Loops 结点,支路和回路
Independent loops ( 独立的回路数 )
A branch represents a single element such as a voltage source or a resistor.
A node is the point of connection between two or more branches.
A loop is any closed path in a circuit.
A mesh ( 网孔) is a loop that contains no other loops within it.
Independent nodes ( 独立的结点数 ) :n-1 1
2 3
4
2.2 Kirchhoff‘s Laws 基尔霍夫定律
b=? n=? l=?b=5 n=3 l=b-n+1=3
Ⅱ. Kirchhoff‘s Laws 基尔霍夫定律
01
N
nni
Kirchhoff’s current law states that the algebraicKirchhoff’s current law states that the algebraic sum sum of currents entering a node (or a closed boundary) is zof currents entering a node (or a closed boundary) is zero.ero.
• Kirchhoff’s current lawKirchhoff’s current law ( KCLKCL 基尔霍夫电流定律)
The sum of the currents entering a node is equal The sum of the currents entering a node is equal to the sum of the currents leaving the node.to the sum of the currents leaving the node.
outin ii
054321 iiiii
52431 iiiii or
Kirchhoff’s voltage law states that the algebraic sum of voltages around a closed path (or loop) is zero.
01
M
mmv
•Kirchhoff’s Kirchhoff’s voltagevoltage law law ( KKVVLL 基尔霍夫电压定律)
015432 vvvvv
or
41532 vvvvv
Sum of voltage drops=Sum of voltage rises
risedrop vv
Example 2.1 Calculate the current i in the circuit
012226 12 ii
0628 2 ii
021 iii
Solution:
For loop 1, KVL gives
For loop 2: KVL gives
At node 1 :
0628 2 ii
then A1i
i1 i2
loop1 loop2
2
1
Ⅰ. Series Resistors and Voltage Division
For N resistors in series
N
nnNeq RRRRR
121
The equivalent resistance of any number of resistors connected in series is the sum of the individual resistances.
2.3 Resistors Combinations
串联电阻和分压
2211 iRviRv
)( 2121 RRivvv
voltage division (分压)
vRR
Rvv
RR
Rv
21
22
21
11
,
21 RR
vi
Then
Ⅱ. Parallel Resistors and Current Division 并联电阻和分流
The equivalent resistance of N resistors connected in parallel:
Neq RRRR /1/1/1/1 21
The equivalent conductance of resistors connected in parallel is the sum of their individual conductances.
N
nnNeq GGGGG
121
Two resistors in parallel
iRR
Rii
RR
Ri
21
12
21
21
,
current division (分流)
Ⅲ. Wye-Delta Transformations Y- 转换
3
RRY
YRR 3
1 2
3
2R
3R
1R
1 2
3
12R
31R23R
1 2
3
YR YR
YR
1 2
3
R
RR
Balanced Wye-Delta Transformations
部分电路图和内容参考了: 电路基础(第 3 版),清华大学出版社 电路(第 5 版),高等教育出版社 特此感谢!