ch 20-2. model of a real battery a real battery can be modeled as an ideal battery (i.e. voltage...

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CH 20-2

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Page 1: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

CH 20-2

Page 2: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Model of a real battery

A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r.

The voltage across the terminals isV = - Ir

With usage, the internal resistance increases and the voltage across the terminals decreases.

Page 3: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Example

The voltage across a battery is 1.5 V when it is not in a circuit. When connected to a bulb, 0.5 A flows through the battery, and the voltage across the terminals is 1.4 V. What is the internal resistance of the battery?

Page 4: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Ideal Voltage Source

We will treat all batteries as ideal voltage sources. The voltage across its terminals is constant (and therefore does NOT depend on the current through the voltage source). The current through the voltage source can have any value.

Page 5: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Series

When elements are connected in series, one element is connected to another element in such a way that there is only one path for current to flow through the elements. The current through each element is the same.

I I

Page 6: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Total Resistance

For two resistors in series, the total resistance is the sum of the resistances.

R1 R2 Req

Page 7: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Example

A 1.5 V battery is connected to a 6 resistor and a 10 resistor that are in series. What is the current through the battery?

R1 R2

Page 8: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Example

A 1.5 V battery is connected to a 6 resistor and a 10 resistor that are in series. What is the voltage across each resistor?

R1 R2

Page 9: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Voltage Divider

R1 R2

Page 10: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Consider the three resistors and the battery in the circuit shown. Which resistors, if any, are connected in series?

A. R1 and R2

B. R1 and R3

C. R2 and R3

D. R1 and R2 and R3

E. No resistors are connected in series.

Adapted fromDavid Marx

Page 11: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

In the circuit shown here, elements _________ are in series.

A. E2 and E5

B. E3 and E4

C. E4 and E5

D. none of the

above

E1

E3

E5

E2

E4

Page 12: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

In the circuit shown here, the current will always be equal through elements _________.

A. E1 and E3

B. E2 and E5

C. E3 and E4

D. E4 and E5

E. none of the

above

E1

E3

E5

E2

E4

Page 13: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

READING QUESTION

In the arrangement shown, the resistances R1, R2, and R3 are all different. Here are four proposed statements about this arrangement: 1. The current through each individual resistor is equal to the current through point b. 2. The currents through all the individual resistors add up to the current through point b. 3. The voltage across each individual resistor is equal to the voltage between points a and b. 4. The voltages across all the individual resistors add up to the voltage between points a and b. Which of these statements are correct?

A. 1 and 3 B. 1 and 4 C. 2 and 3 D. 2

and 4

R1 R2 R3

•b•a

Page 14: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Parallel

Two elements are connected in parallel if their terminals are connected to each other (on both sides). A voltmeter across each element will read the same voltage.

Page 15: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Total Resistance

For two resistors in parallel, the total resistance is LESS than the sum of the resistances.

Req

R1

R2

Page 16: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Example

A 1.5 V battery is connected to 6 and 10 resistors that are in parallel. What is the current through the battery?

R1

R2

Page 17: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Example

A 1.5 V battery is connected to 6 and 10 resistors that are in parallel. What is the current through each resistor?

R1

R2

Page 18: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Current Divider

R1

R2

Page 19: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Consider the three resistors and the battery in the circuit shown. Which resistors, if any, are connected in parallel?

A. R1 and R2

B. R1 and R3

C. R2 and R3

D. R1 and R2 and R3

E. No resistors are connected in parallel.

Adapted fromDavid Marx

Page 20: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

In the circuit shown here, elements _________ are in parallel.

A. E2 and E3

B. E1 and E3

C. E3 and E5

D. E1, E3, and E5

E. none of the

above

E1

E3

E5

E2

E4

Assume the connecting wires have negligible resistance.

Page 21: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

In the circuit shown here, elements _________ are in parallel.

A. E2 and E3

B. E1 and E3

C. E3 and E5

D. E1, E3, and E5

E. none of the

above

E1

E3

E5

E2

E4

Page 22: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

READING QUESTION

In the arrangement shown, the resistances R1, R2, and R3 are all different. Here are four proposed statements about this arrangement: 1. The current through each individual resistor is equal to the current through point b. 2. The currents through all the individual resistors add up to the current through point b. 3. The voltage across each individual resistor is equal to the voltage between points a and b. 4. The voltages across all the individual resistors add up to the voltage between points a and b. Which of these statements are correct?

A. 1 and 3 B. 1 and 4 C. 2 and 3 D. 2

and 4

R1

R2

R3

•a •b

Page 23: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

R = 0.75R = 9.0

R =3.0

12

3

6.0 V

a bA 50 R =

C 15 R =

B 30 R =

In the above circuit, Which of the following correctly compares the currents IA, IB, and IC passing through the three resistors?

A. IA > IB > IC

B. IC > IB > IA

C. IA > IC > IB

D. None of the above

Page 24: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

Power

Power is change in energy per second (1 J/s = 1 W). In the case of a battery, the power of the battery is the rate that it supplies electrical energy. In the case of a resistor, the power of the resistor is the rate that it dissipates electrical energy (and converts it to thermal energy and light energy).

The brightness of a light bulb depends on its power.

Page 25: CH 20-2. Model of a real battery A real battery can be modeled as an ideal battery (i.e. voltage source) and an internal resistance r. The voltage across

A “50 W” bulb and a “100 W” bulb are connected in parallel with a standard 120 volt ac electrical outlet. The brightness of a light bulb is directly related to the power it dissipates. Therefore, the 100 W bulb appears brighter. How does the brightness of the two bulbs compare when these same bulbs are connected in series with the same outlet?

A. Both bulbs will be equally bright.

B. The “100 W” bulb will be brighter.

C. The “50 W” bulb will be brighter. Adapted fromDavid Marx