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Physics 214: General Physics
Professor:
Ricky J. Sethi
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Sethi Family HomePage » Classes » Phys214 » Daily Lecture Notes » Chapter 7
Lecture Notes for Chapters 7
- Reading Memo Insights: To Be Added
- Summary of Important Equations to understand for the HW:
- I = Q/t
- V = PE/Q
- Ohm's law: V = IR
- Power: P = VI = I2R
- Rserial = R1 + R2
- 1/Rparallel = 1/R1 + 1/R2
- Series: I → same; V → divides up.
- Parallel: I → divides up; V → same
- What is charge?
- In Mechanics, we examined the basic property of matter
called mass
- In ElectroDynamics, the basic concept of matter we will
examine is called charge
- In mechanics, we never really knew just what mass is,
only how it behaves;
in the same way, classical E&M only tells us how charge
behaves, but not what it really is.
- Charge is responsible for electrical & magnetic phenomena
- Represented by q or Q and unit of measure: Coulomb (C)
- Possessed by e-, p+, etc. (+ and -)
- Charge on each is e = 1.6 x 10-19 C
- Transparency 1: Atom becomes ionized when it loses
or gains e- (Fig 7.3, p. 249)
- E.g., when rubbed, friction transfers electrons
- Electric Force and Coulomb's Law:
- Electric force of p+ keeps e- in orbit (like gravitational)
- F =
kQ1Q2/r2, where k = 9 x 109 N-m2/C2
- Force on Q1 is equal and opposite to force on Q2
- Like charges repel (Force is +), unlike attract (Force is -)
- Transparency 2: Just like gravity, distance halved,
Force quadrupled (Fig 7.7, p. 250)
- Mass and charge are both fundamental properties of
matter so not surprising that gravity and coulombic force have
similar forms
- Electric force between e- and p+ is
1039 times as large as gravitational force between them
- Transparency 3: charged object can attract uncharged
object (separation of charges) (Fig 7.8, p. 251)
- The Electric Field
- Just like gravity, electrostatic force is "action at a distance"
- Just like gravitational field, helpful to invoke idea of an Electric Field
- Field is the "agent" of the electrostatic force
(actually virtual photons)
- In mechanics, g determines gravitational field
- Transparency 4: Each line is a line of
force and indicates
direction and magnitude of force that the field would exert on
a positive charge (Fig 7.9, p. 251)
- Action at a distance is inherently
unpalatable... how does it work? How is force
actually transmitted across empty space and
time? Is it instantaneous? That would allow
transmission of information faster than speed of
light!
- So instead, let's just imagine a field, an
abstract, mathematical idea
- Field itself exerts the force
- Place test charge (or mass) at various points
in space around object and map both the direction and
magnitude of the Force... that's the field
- Turns out, this idea of field is actually real
(e.g., gravitational force is actually a warping of
space-time by mass); just like Copernicus initially
proposed heliocentric universe as an abstract,
mathematical simplification only ("We know
Earth is the center, but if we just use this
mathematical model with the Sun at the center, we can make
better predictions" and, lo and behold, it really is a
truer idea)
- Positive charges follow lines of force; Negative charges move
against lines of force
- Field strength indicated by density of field lines
- E = F/Q -- Force Density (just like Pressure
is also a Force Density!)
- The Electric Field itself is exactly what exerts the
force on charged objects (can be produced without electric
charges, a la magnetic fields)
- Electric Current & Resistance
- Electric Circuits and Ohm's Law
- Batteries produce an Electric Field that forces
e- to flow through a circuit → like inducing a
Gravitational Field by changing the incline
- An electric circuit has:
- A power supply
- An electrical device (e.g., a resistor like a bulb)
- Wires (or conductors) to carry the current
- The power supply acts like a "charge pump" -- forces
charges to flow out of one terminal, through the circuit, and
into the other terminal
- Imagine a "sea of electrons" (like the "sea of water" in
a water circuit)
- Pump pushes pre-existing water around; battery pushes
pre-existing electrons
- Flow of water is water current; flow of electrons is
electric current (or electricity)
- Just like in Mechanics, we went from considering Forces to
Energy:
- We can move from the idea of an electric field
and the resulting force on the charges in a wire to
the idea of Energy and Work to quantify the effect
of a power supply
- Batteries cause e- to flow -- i.e.,
Force acts on e-, causing them to move a
distance -- that's Work done by the battery!
- Therefore, batteries give e- energy (this
energy is converted to light and heat in bulb)
- Voltage, V = Work/Q = Potential_Energy/Q = F•d/Q = E•d --
i.e., energy given to e- by the battery
- Units of V are Joules/Coulomb = J/C = Volt
- 9-Volt battery gives 9 joules of energy to
each coulomb of electric charge that it
moves through a circuit
- Voltage is also called electric potential and
ΔV is the Potential Difference
- In Mechanics, PE/m = gh; in Electricity, PE/Q = V = E•d
- In the water analogy, Voltage Difference (and so
Intensity of Electric Field since V =
E•d) is analogous to Pressure Difference
| Water |
Electricity |
| Litre of water |
Coulomb of charge |
| Water Flow is 1 litre/sec |
Electric Current is 1 coulomb/sec (ampere) |
| Pump |
Battery |
| Pipe |
Wire |
Pump pressure:
Increase Rate of Flow of water by
↓
Increasing height (F/m = g•h)
↓
Increases Pressure = F/A = mgh/A
↓
RESULTS in increased Force on each parcel of water
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Voltage:
Increase Rate of Flow of Charge (the current) by
↓
Increasing Potential Difference, V (F•d/Q = E•d)
↓
Increases Electrical Field E = F/Q
↓
RESULTS in increased Force on each moving charge
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- Ohm's Law: I = V/R (only for "Ohmic" elements; but R
= V/I always) → V = IR
- In-class Exercise 1: An electric fan has a
resistance of 30 Ω when the current
in it is 3 A. What is the voltage required for this current? (see p. 261)
| Known |
Unknown |
| R = 30 Ω |
V = ?V |
| I = 3A |
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- Series
- Parallel
- Here's one way to think about these circuit types: imagine that the
individual charges (remember, the flow of charges is
the current) are equivalent to individual hikers that hate
each other (since like charges repel each other). Then, the
Potential (the voltage, V) will be analogous to the height
that they start at. In a series circuit, they follow a
single, narrow path where they have to follow each other, one
after the next. However, they start off at the top of a
mountain and slowly descend.
Each slope can be thought of as a resistor that's in
the circuit. The angle of the slope represents the strength
of the resistor (with a shallow angle representing a weak
resistor and a steep angle representing a strong resistor).
The hikers, just like electrons, will take the path of least
resistance and opt for the path with the shallowest slope (if
at all possible).
In a series circuit, they start off at the top of a mountain
and descend the mountain along a single path as follows:
o o
| |
-ooo-____
| | \ --> 1st Slope/Resistor
| | \
| | \ o o
| | \ | |
| | \_____
| | \
| | \ --> 2nd Slope/Resistor
| | \
--o--__________________\
So the flow of hikers (or the flow of charge, or current)
stays the same because each hiker (or each electron) only has
one single path to follow. So here, the current (or
flow of hikers) stays the same whereas the
voltage (or the height) changes across each
resistor (slope) → i.e., the potential drops
across the resistor (slope) while charge flows
through it.
In a parallel circuit, however, you can imagine the hikers
(that hate each other (since like charges repel each other))
going along a flat plateau (i.e, a flat plain with no hills or
valleys) and hitting a fork in the road:
____________________
o o / /\
| | / / \
-ooo-_______/ / \
| | \ / \---> Slope/Resistor
| | \ / \
| | \______________/ \_________
| | \ / \
| | \ / \
| | \ / \________
| | \ / / |
| | \ / / |
| | \/______________/ |
| | |
--o--________________________________________________________|
Now, the hikers will have the choice of TWO possible paths;
one might take the top, while the other takes the bottom,
path. Then, they'll each go down a slope (or resistor) after
which theey'll go
along the path and meet up when the fork re-converges at the
end. Since the hikers represent electrons, and the motion of
the hikers represents the flow of charges, we can see that the
current divides in a parallel circuit.
However, since the whole path is on a plateau, the
voltage stays the same in a parallel circuit!
- In-class Exercise 2: Three light bulbs are connected
in parallel with a 10-V battery. The resistance of the bulbs are
20 Ω, 10 Ω, and 20 Ω; what is the current produced
by the battery? (see p. 263)
| Known |
Unknown |
| V = 10V |
I = ?A |
| R1 = 20Ω;
R2 = 10Ω; R3 = 20Ω |
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- Power and Energy
- Power = energy per time = energy per coulomb x # coulombs
per time = V x I (units of J/C x C/sec = J/s = Watt)
- When a light bulb is rated at a certain wattage (e.g.,
100 W), remember that its rating is only valid for the
specified voltage (usually, 120-V AC in household circuits
in North America). However, once you know its resistance
and the current, you can always get the power
rating, or wattage, via P = VI = (IR)I = I2R
- Energy = P • t (since P = E/t)
- In-class Exercise 3: If a 1,000 W hair dryer is used
for 2.5 minutes, then how much energy does it consume? (see
p. 268)
| Known |
Unknown |
| t = 2.5mins |
t = ?sec |
| P = 1000W |
E = ?J |
- AC and DC
- Two kinds of current: Alternating and Direct
- Direct Current flows in a fixed direction (+ to -)
- Alternating Current reverses polarity (the polarity of the
terminal reverses from + to - and back again -- the voltage
alternates)
- the e- flow, and thus the current direction, reverses
- Some devices can use either; others one or the other
- Transformers can "step up" or "step down" AC voltages
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