Title: Chapter 18 Electric Currents
1Chapter 18Electric Currents
2Simple Electric Cell
- Two dissimilar metals or carbon rods in acid
- Zn ions enter acid leaving terminal negative
- Electrons leave carbon making it positive
- Terminals connected to external circuit
- Battery referred to several cells originally
3Electric Current
- If we connect a wire between the two terminals
electrons will flow out of the negative terminal
and toward the positive terminal? we have an
electric current. - Electric current I is defined as the net amount
of charge that flows past a given point per unit
time.
- 1 C/s 1A (ampere)
- An ampere is a large current and often currents
are mA (10-3 A) or ?A (10-6 A).
4Electric Circuit
- It is necessary to have a complete circuit in
order for current to flow. - The symbol for a battery in a circuit diagram is
5Conventional current direction is opposite to
actual electron flow direction which is to .
6Ohms Law
- For wires and other circuit devices, the current
is proportional to the voltage applied to its
ends - I ?
V - The current also depends on the amount of
resistance that the wire offers to the electrons
for a given voltage V. We define a quantity
called resistance R such that - V I R (Ohms Law)
- The unit of resistance is the ohm which is
represented by the Greek capital omega (?). - Thus
7Resistors
- A resistor is a circuit device that has a fixed
resistance.
Resistor
Circuit symbol
Resistors obey Ohms law but not all circuit
devices do (semi-conductor diode, LED)
Resistor
non-ohmic device
8Example A person experiences a mild shock if a
current of 80 ?A flows along a path between the
thumb and the index finger. The resistance of
this path is 4.0x105 ? when the skin is dry and
2000 ? when the skin is wet. Calculate the
minimum voltage difference between these two
points that will produce a mild shock.
9Example A person experiences a mild shock if a
current of 80 ?A flows along a path between the
thumb and the index finger. The resistance of
this path is 4.0x105 ? when the skin is dry and
2000 ? when the skin is wet. Calculate the
minimum voltage difference between these two
points that will produce a mild shock.
10Example Calculate the number of electrons per
second that flow past a point on the skin in the
previous example.
11Example Calculate the number of electrons per
second that flow past a point on the skin in the
previous example.
12Power in Electric Circuits
- Electrical circuits can transmit and consume
energy. - When a charge Q moves through a potential
difference V, the energy transferred is QV. - Power is energy/time and thus
and thus
13Notes on Power
- The formula for power applies to devices that
provide power such as a battery as well as to
devices that consume or dissipate power such as
resistors, light bulbs and electric motors.
- For ohmic devices, the formula for power can be
combined with Ohms Law to give other versions
14Household Power
- Electric companies usually bill by the
kilowatt-hour (kWh.) which is the energy consumed
by using 1.0 kW for one hour. - Thus a 100 W light bulb could burn for 10 hours
and consume 1.0 kWh. - Electric circuits in a building are protected by
a fuse or circuit breaker which shuts down the
electricity in the circuit if the current exceeds
a certain value. This prevents the wires from
heating up when carrying too much current.
15Connection of Household Appliances
16- Example A person turns on a 1500 W electric
heater, a 100 W hair dryer and then a 300 W
stereo. All of these devices are connected to a
single 120 V household circuit that is connected
to a 20 A circuit breaker. At what point will the
circuit breaker trip off?
17- Example A person turns on a 1500 W electric
heater, a 100 W hair dryer and then a 300 W
stereo. All of these devices are connected to a
single 120 V household circuit that is connected
to a 20 A circuit breaker. At what point will the
circuit breaker trip off?
18- Example If electricity costs 0.1379 per kWh in
Nova Scotia, calculate the cost of operating all
the appliances in the previous problem for 2.0
hours.
19- Example If electricity costs 0.1379 per kWh in
Nova Scotia, calculate the cost of operating all
the appliances in the previous problem for 2.0
hours.
20Microscopic View of Current
- Read Example 18-13 on page 545. It studies a
5.0A current in a copper wire that is 3.2 mm in
diameter. It finds that the average free
electron moves with a velocity of 4.7 x 10-5 m/s
in the direction of the current. This is called
the drift velocity. - It also assumes the free electrons behave like
an ideal gas and calculates that the thermal
velocity of the average electron is 1.2 x 105
m/s. - Thus in a wire carrying a current, the electron
motion is largely random with a slight tendency
to move in the direction of the current. Thus if
you could see electrons in a wire carrying
current they would appear to be moving randomly.
21Summary of Units
22Chapter 19
23EMF
- Devices that supply energy to an electric circuit
are referred to as a source of electromotive
force. Since this name is misleading, we just
refer to them as source of emf (symbolized by ?
and a slightly different symbol in the book.) - Sources of emf such as batteries often have
resistance which is referred to as internal
resistance.
24Terminal Voltage
- We can treat a battery as a source of ? in series
with an internal resistor r. - When there is no current then the terminal
voltage is Vab ? - But with current I we have
- The internal resistance is small but increases
with age.
25Circuit Symbols
26Resistors in Series - Derivation
- We want to find the single resistance Req that
has the same effect as the three resistors R1,
R2, and R3. - Note that the current I is the same throughout
the circuit since charge cant accumulate
anywhere. - V is the voltage across the battery and also
- V V1 V2 V3
- Since V1 I R1 etc., we can say
The equivalent equation is VIReq and thus
27Summary - Resistors in Series
The current I is the same throughout the circuit
since charge cant accumulate anywhere.
28Resistors in Parallel - Derivation
- This is called a parallel circuit
- Notice V1 V2 V3 V
- Since charge cant disappear, we can say
- We can combine these equations with
- V IReq to give
29Summary - Resistors in Parallel
- The electric potential (voltage) is the same
across each resistor - V1 V2 V3
- The current through the battery splits several
ways - I I1 I2 I3
- Can be 2, 3 or more resistors in parallel.
30Example A 3.0 V battery is connected to three
resistors as shown. Calculate the resistance of
the equivalent circuit and the power dissipated
in the equivalent circuit. R1 500 O, R2 1000
O and R3 2000 O.
31Example A 3.0 V battery is connected to three
resistors as shown. Calculate the resistance of
the equivalent circuit and the power dissipated
in the equivalent circuit. R1 500 O, R2 1000
O and R3 2000 O.
32Example From the previous example, calculate the
current and the power dissipated in each resistor
and the total power dissipated in the circuit.
33Example From the previous example, calculate the
current and the power dissipated in each resistor
and the total power dissipated in the circuit.
34Example A 3.0 V battery is connected to 4
resistors as shown. Calculate the resistance of
the equivalent circuit and the current in the
equivalent circuit. R1 500 O, R2 1000 O, R3
1000 O, and R4 2000 O.
35Example A 3.0 V battery is connected to 4
resistors as shown. Calculate the resistance of
the equivalent circuit and the current in the
equivalent circuit. R1 500 O, R2 1000 O, R3
1000 O, and R4 2000 O.
36Ammeter
- To measure current ammeter must be connected in
series. - Must have small internal resistance or it will
reduce current and give a faulty measurement.
37Voltmeters
- To measure voltage difference, it must be
connected in parallel. - Must have high internal resistance or it will
draw too much current which reduces voltage
difference and gives a faulty measurement.