10. Resistor circuits. Kirchhoff's laws

University of Rhode Island University of Rhode Island

DigitalCommons@URI DigitalCommons@URI

PHY 204: Elementary Physics II -- Slides PHY 204: Elementary Physics II (2021)

2020

10. Resistor circuits. Kirchhoff's laws 10. Resistor circuits. Kirchhoff's laws

Gerhard Müller University of Rhode Island, [email protected]

Robert Coyne University of Rhode Island, [email protected]

Follow this and additional works at: https://digitalcommons.uri.edu/phy204-slides

Creative Commons License

This work is licensed under a Creative Commons Attribution-Noncommercial-Share Alike 4.0

License.

Recommended Citation Recommended Citation Müller, Gerhard and Coyne, Robert, "10. Resistor circuits. Kirchhoff's laws" (2020). PHY 204: Elementary Physics II -- Slides. Paper 35. https://digitalcommons.uri.edu/phy204-slides/35https://digitalcommons.uri.edu/phy204-slides/35

This Course Material is brought to you for free and open access by the PHY 204: Elementary Physics II (2021) at DigitalCommons@URI. It has been accepted for inclusion in PHY 204: Elementary Physics II -- Slides by an authorized administrator of DigitalCommons@URI. For more information, please contact [email protected].

Direct Current Circuit

Consider a wire with resistance R = ρ`/A connected to a battery.

• Resistor rule: In the direction of I across a resistor with resistance R, the electric potential drops:∆V = −IR.

• EMF rule: From the (−) terminal to the (+) terminal in an ideal source of emf, the potential rises: ∆V = E .• Loop rule: The algebraic sum of the changes in potential encountered in a complete traversal of any loop

in a circuit must be zero: ∑ ∆Vi = 0.

+ −emf

I

+ −emf

I

I

R

a b

ε

a b a

Va

Vb

−IR ε+ −

I

a b

circuit diagramphysical system electric potential

tsl143

Battery with Internal Resistance

• Real batteries have an internal resistance r.• The terminal voltage Vba ≡ Va −Vb is smaller than the emf E written on the label if a current flows

through the battery.• Usage of the battery increases its internal resistance.

• Current from loop rule: E − Ir− IR = 0 ⇒ I =E

R + r

• Current from terminal voltage: Vba = E − Ir = IR ⇒ I =VbaR

+ −emf

I

+ −emf

IR

ba

εI

r+ −

I

a b

electric potentialphysical system circuit diagram

a b

−Ir

a

Va

Vb

ε

−IR

.

tsl144

Resistor Circuit (4)

Consider the resistor circuit shown.

(a) Find the direction of the positive current (cw/ccw).(b) Find the magnitude of the current.(c) Find the voltage Vab = Vb −Va.(d) Find the voltage Vcd = Vd −Vc.

1Ω

12V

1Ω

2Ω

a

cd

b

tsl151

Resistor Circuit (6)

Consider the resistor circuit shown.

(a) Choose a current direction and use the loop rule to determine the current.(b) Name the direction of positive current (cw/ccw).(c) Find Vab ≡ Vb −Va along two different paths.

b

a

1Ω

6V

1Ω 18V

2Ω

24V

2Ω12V

tsl153

Power in Resistor Circuit

Battery in use• Terminal voltage: Vab = E − Ir = IR

• Power output of battery: P = VabI = E I− I2r

• Power generated in battery: E I• Power dissipated in battery: I2r

• Power transferred to load: P = I2R

b

a

ε

rR

Battery being charged:

• Terminal voltage: Vab = E + Ir

• Power supplied by charging device: P = VabI

• Power input into battery: P = E I + I2r

• Power stored in battery: E I• Power dissipated in battery: I2r

b

a

chargingdevice

ε

r

tsl154

Resistor Circuit (7)

Consider two 24V batteries with internal resistances (a) r = 4Ω, (b) r = 2Ω.

• Which setting of the switch (L/R) produces the larger power dissipation in the resistor on the side?

L R

24V

4Ω

2Ω

L R

24V

2Ω4Ω 4Ω

2Ω

(a) (b)

tsl155

Impedance Matching

A battery providing an emf E with internal resistance r is connected to an external resistor of resistance R asshown.

For what value of R does the battery deliver the maximum power to the external resistor?

• Electric current: E − Ir− IR = 0 ⇒ I =E

R + r

• Power delivered to external resistor: P = I2R =E2R

(R + r)2 =E2

rR/r

(R/r + 1)2

• Condition for maximum power: dPdR

= 0 ⇒ R = r

R

εr

I

tsl156

Resistor Circuit (5)

Consider the resistor circuit shown.

(a) Choose a current direction and use the loop rule to determine the current.(b) Name the direction of positive current (cw/ccw).(c) Find the potential difference Vab = Vb −Va.(d) Find the voltage Vcd = Vd −Vc.

12V2Ω

7Ω3Ω

4Ω 4V

c

a

b

d

tsl152

Symbols Used in Cicuit Diagrams

A

V

ε

L

C

R

C

B

E

resistor

capacitor

inductor

emf source

ammeter (connect in series)

voltmeter (connect in parallel)

diode

transistor

tsl158

Resistors Connected in Series

Find the equivalent resistance of two resistors connected in series.

• Current through resistors: I1 = I2 = I

• Voltage across resistors: V1 + V2 = V

• Equivalent resistance: R ≡ VI=

V1

I1+

V2

I2

• ⇒ R = R1 + R2

V0

V1

V2

x

V + V00V

2RR1

I I

tsl146

Resistors Connected in Parallel

Find the equivalent resistance of two resistors connected in parallel.

• Current through resistors: I1 + I2 = I

• Voltage across resistors: V1 = V2 = V

• Equivalent resistance: 1R≡ I

V=

I1

V1+

I2

V2

• ⇒ 1R

=1

R1+

1R2

V0

V = V2

x

x

V

V = VV

0

0V + V

0

1

R

R2

1I

I2

1

tsl145

Resistor Circuit (1)

Consider the two resistor circuits shown.

(a) Find the resistance R1.(b) Find the emf E1.(c) Find the resistance R2.(d) Find the emf E2.

1AR1

1Ω 2Ω

1Ω

1A

2A

6Ω

R2

ε2ε1

2A

tsl148

Resistor Circuit (2)

Consider the two resistor circuits shown.

(a) Find the resistance R1.(b) Find the current I2.(c) Find the current I3.(d) Find the resistance R4.

3A

6Ω

R1Ω1

I2

12V 12V

3Ω

3A 2Ω

I3R4

tsl149

Resistor Circuit (8)

Consider the circuit of resistors shown.

• Find the equivalent resistance Req.• Find the currents I1, . . . , I5 through each resistor and the voltages V1, . . . , V5 across each resistor.• Find the total power P dissipated in the circuit.

4Ω

6Ω

12Ω

3Ω 5Ω

12V

R = R =

R =

R =

R =1

2

3

4 5

ε =

tsl157

Kirchhoff’s Rules

Loop Rule

• When any closed-circuit loop is traversed, the algebraic sum of the changes in electric potential must bezero.

Junction Rule

• At any junction in a circuit, the sum of the incoming currents must equal the sum of the outgoing currents.

Strategy

• Use the junction rule to name all independent currents.• Use the loop rule to determine the independent currents.

tsl159

Applying the Junction Rule

In the circuit of steady currents, use the junction rule to find the unknown currents I5, . . . , I9.

Ι 8Ι

ε+

Ι

Ι Ι

−

1

2

5

3

6

79

4

I = 4A

I = 9A

I = 3A

I = 1A

tsl160

Applying Kirchhoff’s Rules

Consider the circuit shown below.

• Junction a: I1, I2 (in); I1 + I2 (out)• Junction b: I1 + I2 (in); I1, I2 (out)• Two independent currents require the use of two loops.• Loop A (ccw): 6V− (2Ω)I1 − 2V− (2Ω)I1 = 0

• Loop B (ccw): (3Ω)I2 + 1V + (2Ω)I2 − 6V = 0

• Solution: I1 = 1A, I2 = 1AI2

1

A2V 6V

2Ω 1I

2

b

aI + I

I + I

1 2

B

Ω2

2Ω I1 I2 Ω3

1V

tsl161

Resistor Circuit (11)

Consider the electric circuit shown.

• Identify all independent currents via junction rule.• Determine the independent currents via loop rule.• Find the Potential difference Vab = Vb −Va.

b

a

1Ω

4V 4V

2Ω

2V

1Ω

1Ω

1Ω

tsl164

Resistor Circuit (9)

Use Kirchhoff’s rules to find

(a) the current I,(b) the resistance R,(c) the emf E ,(d) the voltage Vab ≡ Vb −Va.

b

a

I

18V

R

1A

2Ω

ε

6A

2Ω

tsl162

Resistor Circuit (10)

Consider the electric circuit shown.

(a) Find the current through the 12V battery.(b) Find the current through the 2Ω resistor.(c) Find the total power dissipated.(d) Find the voltage Vcd ≡ Vd −Vc.(e) Find the voltage Vab ≡ Vb −Va.

a

b

3Ω

1Ωc

4V

d1Ω

2Ω12V

tsl163

Resistor Circuit (12)

Consider the electric circuit shown.

• Find the equivalent resistance Req of the circuit.• Find the total power P dissipated in the circuit.

1Ω

1Ω

2Ω

2Ω

3Ω

13V

tsl165

Resistor Circuit (3)

Consider the rsistor and capacitor circuits shown.

(a) Find the equivalent resistance Req.(b) Find the power P2, P3, P4 dissipated in each resistor.(c) Find the equivalent capacitance Ceq.(d) Find the energy U2, U3, U4 stored in each capacitor.

3Ω

2Ω 4Ω 2nF 4nF

3nF

12V12Vtsl150