physics for scientists and engineers, 6e chapter 28 – direct current circuits

29
Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Upload: taya-fawcett

Post on 31-Mar-2015

237 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Physics for Scientists and Engineers, 6e

Chapter 28 – Direct Current Circuits

Page 2: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In order to maximize the percentage of the power that is delivered from a battery to a device, the internal resistance of the battery should be

1 2 3

33% 33%33%

1 2 3 4 5

1. as low as possible

2. as high as possible

3. The percentage does not depend on the internal resistance.

Page 3: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Power is delivered to the internal resistance of a battery, so decreasing the internal resistance will decrease this “lost” power and increase the percentage of the power delivered to the device.

Page 4: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In the figure below, imagine positive charges pass first through R1 and then through R2. Compared to

the current in R1, the current in R2 is

1 2 3 4 5

1. smaller

2. larger

3. the same

1 2 3

33% 33%33%

Page 5: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In a series circuit, the current is the same in all resistors in series. Current is not “used up” as charges pass through a resistor.

Page 6: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

If a piece of wire is used to connect points b and c in Figure 28.4b, the brightness of bulb R1 will

1 2 3

33% 33%33%

1 2 3 4 5

1. increase

2. decrease

3. remain the same

Page 7: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Connecting b to c “shorts out” bulb R2 and

changes the total resistance of the circuit from R1 + R2 to just R1. Because the resistance of the

circuit has decreased (and the emf supplied by the battery does not change), the current in the circuit increases.

Page 8: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

With the switch in this circuit closed (left), there is no current in R2,

because the current has an alternate zero-resistance path through the switch. There is current in R1 and this current is measured with the

ammeter (a device for measuring current) at the right side of the circuit. If the switch is opened (Fig. 28.5, right), there is current in R2.

What happens to the reading on the ammeter when the switch is opened?

1 2 3

33% 33%33%

1 2 3 4 5

1. the reading goes up

2. the reading goes down

3. the reading does not change

Page 9: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

When the switch is opened, resistors R1

and R2 are in series, so that the total circuit

resistance is larger than when the switch was closed. As a result, the current decreases.

Page 10: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In this figure, imagine that we add a third resistor in series with the first two. The current in the battery will:

1 2 3

33% 33%33%

1 2 3 4 5

1. increase

2. decrease

3. remain the same

Page 11: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Adding another series resistor increases the total resistance of the circuit and thus reduces the current in the circuit.

Page 12: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In the same figure, imagine that we add a third resistor in series with the first two. The terminal voltage of the battery will

1 2 3

33% 33%33%

1 2 3 4 5

1. increase

2. decrease

3. remain the same

Page 13: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

The potential difference across the battery terminals increases because the reduced current results in a smaller voltage decrease across the internal resistance.

Page 14: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In the figure below, imagine that we add a third resistor in parallel with the first two. The current in the battery will:

1 2 3

33% 33%33%

1 2 3 4 5

1. increase

2. decrease

3. remain the same

Page 15: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

If the second resistor were connected in parallel, the total resistance of the circuit would decrease, and the current in the battery would increase.

Page 16: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In the same figure, imagine that we add a third resistor in parallel with the first two. The terminal voltage of the battery will:

1 2 3

33% 33%33%

1 2 3 4 5

1. increase

2. decrease

3. remain the same

Page 17: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

The potential difference across the terminals would decrease because the increased current results in a greater voltage drop across the internal resistance.

Page 18: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

With the switch in the following circuit open (left), there is no current in R2. There is current in R1 and this current is

measured with the ammeter at the right side of the circuit. If the switch is closed (right), there is current in R2. What happens to

the reading on the ammeter when the switch is closed?

1 2 3

33% 33%33%

1 2 3 4 5

1. the reading goes up

2. the reading goes down

3. the reading does not change

Page 19: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

When the switch is closed, resistors R1 and

R2 are in parallel, so that the total circuit

resistance is smaller than when the switch was open. As a result, the current increases.

Page 20: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

In using Kirchhoff’s rules, you generally assign a separate unknown current to

1 2 3 4

25% 25%25%25%

1 2 3 4 5

1. each resistor in the circuit

2. each loop in the circuit

3. each branch in the circuit

4. each battery in the circuit

Page 21: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

A current is assigned to a given branch of a circuit. There may be multiple resistors and batteries in a given branch.

Page 22: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Consider the circuit seen below and assume that the battery has no internal resistance. Just after the switch is closed, the potential difference across which of the following is equal to the emf of the battery?

1 2 3

33% 33%33%

1 2 3 4 5

1. C

2. R

3. neither C nor R

Page 23: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Just after the switch is closed, there is no charge on the capacitor, so there is no voltage across it. Charges begin to flow in the circuit to charge up the capacitor, so that all of the voltage ΔV = IR appears across the resistor.

Page 24: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

After a very long time, the potential difference across which of the following is equal to the emf of the battery?

1 2 3

33% 33%33%

1 2 3 4 5

1. C

2. R

3. neither C nor R

Page 25: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

After a long time, the capacitor is fully charged and the current drops to zero. Thus, the battery voltage is now entirely across the capacitor.

Page 26: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Consider the circuit in the figure below and assume that the battery has no internal resistance. Just after the switch is closed, the current in the battery is

1 2 3 4 5

20% 20% 20%20%20%

1 2 3 4 5

1. zero

2. ε/2R

3. 2ε /R

4. ε/R

5. impossible to determine.

Page 27: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

Just after the switch is closed, there is no charge on the capacitor. Current exists in both branches of the circuit as the capacitor begins to charge, so the right half of the circuit is equivalent to two resistances R in parallel for an equivalent resistance of 1/2R.

Page 28: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

After a very long time, the current in the battery is

1 2 3 4 5

20% 20% 20%20%20%

1 2 3 4 5

1. zero

2. ε/2R

3. 2ε /R

4. ε/R

5. impossible to determine.

Page 29: Physics for Scientists and Engineers, 6e Chapter 28 – Direct Current Circuits

After a long time, the capacitor is fully charged and the current in the right-hand branch drops to zero. Now, current exists only in a resistance R across the battery.