Industrial Electronics. Fundamentals of Electric Circuits презентация

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Chapter 1 Fundamentals of Electric Circuits Circuit is a current

Chapter 1
Fundamentals of Electric Circuits

Circuit is a current path,

it is needed for some electrical equipment by certain
Or elements combined in a certain way up.
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Circuit R, I, U, C, L, etc. Current I Voltage

Circuit R, I, U, C, L, etc.
Current I
Voltage V
Charge Q=I*t
Resistance

resistor R
Capacitance capacitor C
Inductance inductor L
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Learning Objectives: Identify the principal elements of electric circuits: nodes,

Learning Objectives:
Identify the principal elements of electric circuits:
nodes, loops, meshes,

branches, voltage and current sources;
Apply Kirchhoff’s laws to simple electric circuits and derive the basic circuit equations.
Compute the power delivered or absorbed by circuit elements.
Apply the voltage and current divider laws to calculate unknown variables in simple series, parallel, and series-parallel circuits.
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§1 Fundamentals of Electric Circuits The resistor The inductor The

§1 Fundamentals of Electric Circuits

The resistor
The inductor
The capacitor

§ 1-1 1.

Circuit models(电路模型)

Two active(有源)models

Three passive(无源)models

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The voltage independent source The current independent source The ideal

The voltage independent source

The current independent source

The ideal voltage source:

Independent Sources

V

= E – R0 I

V0 = E

Is =

  When R0 = 0, V = E, the source is called ideal voltage source.

R0 = 0

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V0 = IS R0 IS R0 = ∞ When R0

V0 = IS R0

IS

R0 = ∞

When R0 = ∞ ,

I = IS, the source is called ideal current source.

The ideal current source:

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(CCVS) (VCCS) (CCCS) (VCVS) Dependent (Controlled) Sources

(CCVS)

(VCCS)

(CCCS)

(VCVS)

Dependent (Controlled) Sources

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2. Network variables (网络变量) The systems of units (单位制) :

2. Network variables (网络变量)

The systems of units (单位制) : International system

of units; SI unit
Length [meter] (m) Mass [kilogram] (kg)
Time [second] (s)

(1) Current -- i(t), I ---- (A, mA, μA...)
The net time-rate of transference (传递) of charge is referred to as the flow of current.

(2) Energy (or work) -- w(t) (J)

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(4) Power -- p(t) (W, kW, mW) The time rate

(4) Power -- p(t) (W, kW, mW)

The time rate of

performing work is defined as power.
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7 3. Reference directions(参考方向) (1) Reference directions for current (2)

7

3. Reference directions(参考方向)

(1) Reference directions for current

(2) Reference directions for voltage


: Electron: negatively charged
Direction of current: is defined as the flow direction of positive charge.

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7 (3) Reference conventions (惯例) for two-terminal elements (R, L,

7

(3) Reference conventions (惯例) for two-terminal elements (R, L, C or

... )

The relative (关联) reference directions

The reference arrow for the current variable enters the terminal, which is identified by the plus sign of the voltage reference polarity markings.

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(4) The reference for power p(t) p(t)>0 the power absorbed by the element.

(4) The reference for power

p(t)<0 the negative power absorbed by the

element, or it is actually generating power and delivering it to some external element.

p(t)>0 the power absorbed by the element.

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§1-2 Ohm's law Ohm's law states that voltage across many

§1-2 Ohm's law

Ohm's law states that voltage across many types

of conducting materials is directly proportional to the current flowing through the material.

The resistor is a passive element that cannot deliver power or store energy.

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The current through and voltage across a resistor must both

The current through and voltage across a resistor must both

vary with time in the same manner.

We define a "short circuit" as a resistance of zero ohms.

We define a "open circuit" as an infinite resistance.

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§1-3 Kirchhoff's laws A point at which three or more

§1-3 Kirchhoff's laws

A point at which three or more elements

have common connection is called a node(节点).

Suppose that we start at one node in a network and move through a simple element to the node at the other…, if no node was encountered more than once, then the set of nodes and elements that we have passed through is defined as a path(路径).

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We define a branch(支路) as a single path in a


We define a branch(支路) as a single path in

a network, composed of one simple element (or more elements ) and the nodes at each end of that element.

Kirchhoff's current law --KCL

The algebraic sum of all the currents entering any node is zero.

If the node at which we started is the same as the node on which we ended, then the path is a closed path(闭合路径)or a loop(回路).

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The algebraic sum of all the currents leaving a node


The algebraic sum of all the currents leaving a

node is zero.
or: The algebraic sum of all the currents entering a node must equal the algebraic sum of all the currents leaving the node.

The three equivalent equations

The algebraic sum of all the currents entering any node is zero.

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KCL: The KCL may be extended to the supernode.

KCL:

The KCL may be extended to the supernode.

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A mesh (网孔)is a loop that does not contain other

A mesh (网孔)is a loop that does not contain other loops.

Loop1

Loop2

Loop3

3

loops: loop1, loop2, loop3;
2 meshes: loop1, loop2
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基尔霍夫电流定律(KCL) Example: Solution: KCL: I1 – I2+ I3 + I4

基尔霍夫电流定律(KCL)

Example:

Solution:
KCL: I1 – I2+ I3 + I4 = 0

Known quantities: I1=

9 A, I2 = –2 A,I4 = 8 A.
Determine the current I3 .

9 –( – 2)+ I3 + 8 = 0

I3 = –19 A

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The algebraic sum of the voltage around any closed path

The algebraic sum of the voltage around any closed path

in a circuit is zero.

Kirchhoff's voltage law--KVL

KVL:

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Voltage divider Equivalent series resistance R i + – §1-4 Series resistors and voltage divider rule

Voltage divider

Equivalent series resistance

R

i

+


§1-4 Series resistors and voltage divider rule

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Current divider Equivalent parallel resistance R i + – §1-5 Parallel resistors and current divider rule

Current divider

Equivalent parallel resistance

R

i

+


§1-5 Parallel resistors and current divider rule

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Current divider Equivalent parallel resistance

Current divider

Equivalent parallel resistance

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§1-6 Source transformations The ideal voltage source and a series

§1-6 Source transformations

The ideal voltage source and a series resistance

comprise a practical voltage source.

A practical current source is defined as an ideal current source in parallel with an internal resistance Rsi.

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We shall define two sources as being equivalent if each

We shall define two sources as being equivalent if each

produces identical current and identical voltage in any loads which is placed across its terminals.

Conditions of equivalence:

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