Ee204 01 DC Review

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Electrical Engineering course. Dc Review on ohm's law, circuit analysis, kirchoff's law.

Transcript of Ee204 01 DC Review

EE 204 Basic Electronics and Electrical Power

Chapter 1: DC Review

EE 204 Chapter 1: DC Review 1

Some Useful Analogies

• E(V) Voltage ~ Pressure Æ causes ‘something’ to flow • I(A) Current ~ ‘something’ Æ water, charge, flux • R(Ω) Resistance ~ ‘restriction’ Æ prevents the flow

EE 204 Chapter 1: DC Review 2

Resistor in Direct Current (DC) Circuits

• Ohm’s Law:

• Voltage in Volts (V) • Current in Amperes (A) • Resistance in Ohms (Ω)

• Will see “E” used instead of “V” when referring to the voltage

of a source (e.g. battery)

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V I RVoltage Current Resistance u

u

Resistors in Parallel

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1 1 1

1

1

6 16

E I RV II A

u

u :

1 2 2

2

2

6 32

E I RV II A

u

u :

Resistors in Series

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1 1 2

1

6 1 31.5

E I R I RV I II A

u u

u : u :

Kirchhoff’s Voltage Law

• The total sum of the voltage rises and drops around a closed loop must be zero:

• In a passive component like a resistor (a sink for the energy), the voltage is higher on the input end (current), and lower” on the output

• For a source of energy like a battery however, the current flows out of the positive terminal and back into the negative terminal

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0V ¦

Example 1

• What is the voltage across Resistor R5?

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Example 1 Solution

• Consider two loop currents I2 and I3:

• Using KVL on the middle loop:

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I1 I2 I3

2 2 5 2 3 1

2 2 3

2 3

0

6 2 12 0

8 2 12 0 Eq.1

R I R I I E

I I I V

I I V

: :

: : m

Example 1 Solution (cont.)

• Using KVL on the right loop:

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I1 I2 I3

3 3 6 3 2 5 3 2

3 3 3 2

2 3

0

3 3 4 2 0

2 8 4 0 Eq.2

R I R I E R I I

I I V I I

I I V

: : :

: : m

Example 1 Solution (cont.)

• Determine I3:

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2 3

2 3

3

3

3

8 2 12 0

8 32 16 0

30 4 0

30 40.133

I I V

I I V

I V

I VI A

: :

: :

:

:

Using Eq.1Using Eq.2×4Eq.1 + Eq.2 4

m

m

m u

Example 1 Solution (cont.)

• Determine I2:

• Determine VR5:

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2 3

2

2

2

8 2 12 0

8 2 0.133 12 0

8 11.7341.466

I I V

I A V

I VI A

: :

: :

:

5

5

5

5 2 3

2 1.466 0.133

3.2 positive voltageon top

R

R

R

V R I I

V A A

V V

:

Thévenin’s Theorem

• Any linear electrical network with voltage and current sources and only resistances can be replaced at terminals A-B by an equivalent voltage source Vth in series with an equivalent resistance Rth

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Thévenin’s Theorem (cont.)

• The equivalent voltage Vth is the voltage obtained at terminals A-B of the network with terminals A-B open circuited

• The equivalent resistance Rth is the resistance obtained at terminals A-B of the network will all its independent current sources open circuited and all its independent voltage sources short circuited

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Example 2

• Determine the voltage across Resistor R5 using Thévenin’s Theorem

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Example 2 Solution

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3 62 1 2

2 3 6

3 34 12 46 3 3

8

th ab

th

th

R RV V E E ER R R

V V V V

V V

§ · ¨ ¸ © ¹

: :§ · ¨ ¸: : :© ¹

Example 2 Solution (Cont.)

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2 3 62 3 6

2 3 6

6 3 33

6 3 3

th

th

R R RR R R R

R R R

R

: : : :

: : :

Example 2 Solution (Cont.)

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5

5

5

5

5

2 83 2

3.2 positive voltageon top

R thth

R

R

RV VR R

V V

V V

u

: u

: :

Norton’s Theorem

• Any linear electrical network with voltage and current sources and only resistances can be replaced at terminals A-B by an equivalent current source Ino in parallel with an equivalent resistance Rno

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Norton’s Theorem (cont.)

• The equivalent current Ino is the current obtained at terminals A-B of the network with terminals A-B short circuited

• The equivalent resistance Rno is the resistance obtained at terminals A-B of the network will all its independent current sources open circuited and all its independent voltage sources short circuited (note that this is the same as calculating the Thévenin equivalent resistance)

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Example 3

• Determine the voltage across Resistor R5 using Norton’s Theorem

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Example 3 Solution

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1 2

2 3 6

12 46 3 32.667

no ab

no

no

E EI IR R R

V VI

I A

: : :

Example 3 Solution (Cont.)

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2 3 62 3 6

2 3 6

6 3 33

6 3 3

no

no

R R RR R R R

R R R

R

: : : :

: : :

Example 3 Solution (Cont.)

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5

5

5

5

5 5

55

3 2.667 23 2

3.2 positive voltageon top

R

noR no

no

R

R

V I R

RV I RR R

V A

V V

u

§ · u u¨ ¸© ¹§ ·:

u u :¨ ¸: :© ¹

Power Dissipated in a Resistor

• The power (P) dissipated in a resistor is given by:

𝑃 = 𝑉 × 𝐼

• Making use of Ohm’s law (𝑉 = 𝐼 × 𝑅):

𝑃 = 𝐼 𝑅

𝑃 =𝑉𝑅

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KVL Review:

• What is the voltage across R2? • 3V 4V 6V 20V

• What is the current through R3? • 1.2A 10A .30A 3.33A

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KCL Review

• What is the current through R2? • .5A 1A 2A 2.5A

• What is the total current coming from the source, E? • .5A 1.5A 2.5A 3.5A

• What is the voltage across R3? • 2V 10V 12V 5V

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Thévenin Review

• What is the Thévenin Voltage? • 3.33V 6.67V 10V 20V

• What is the Thévenin resistance? • 6.67 Ohms 10 Ohms 20 Ohms 26.67 Ohms

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