PHYSICS HSC NOTES

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Space
Weight force on an object due to gravitational field
π‘€π‘’π‘–π‘”β„Žπ‘‘ = π‘šπ‘Žπ‘ π‘  × 9.8
Projectile Motion
Galileo’s analysis of projectile motion
1.
Vertical motion is independent of horizontal motion
2.
Horizontally the speed is constant
3.
Vertically acceleration is uniform ( = 9.8m/s/s)
Analysing and calculating projectile motions
Step:
1.
Work out horizontal and vertical components of initial velocity
Calculate vertical flight time using 𝑣
2.
Vsinπœƒ
V
πœƒ
= 𝑒 + π‘Žπ‘‘
Vcosπœƒ
u = Vsinπœƒ
v= 0
a = 9.8m/s/s
t = ½ of flight time
Using Vertical flight time to calculate range using 𝑑 = 𝑣 × π‘‘
t = flight time
v = Vcosπœƒ
d = horizontal distance object travels.
3.
Maximum range
Vertical Analysis
𝑣 = 𝑒 + π‘Žπ‘‘
0 = π‘‰π‘ π‘–π‘›πœƒ − 𝑔𝑑
𝑔𝑑 = π‘‰π‘ π‘–π‘›πœƒ
𝑑=
Vsinπœƒ
𝑔 = 9.8π‘š/𝑠/𝑠
𝑑 = π‘‘π‘–π‘šπ‘’ π‘‘π‘Žπ‘˜π‘’π‘› π‘‘π‘œ π‘Ÿπ‘’π‘Žπ‘β„Ž max π‘–π‘šπ‘’π‘š β„Žπ‘’π‘–π‘”β„Žπ‘‘
π‘‰π‘ π‘–π‘›πœƒ
𝑔
π‘‘π‘‘π‘œπ‘‘π‘Žπ‘™ =
2π‘‰π‘ π‘–π‘›πœƒ
π‘‘π‘‘π‘œπ‘‘π‘Žπ‘™ = π‘“π‘™π‘–π‘”β„Žπ‘‘ π‘‘π‘–π‘šπ‘’
𝑔
Horizontal analysis
π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’
𝑆𝑝𝑒𝑒𝑑 =
π‘‘π‘–π‘šπ‘’
𝑅
π‘‰π‘π‘œπ‘ πœƒ = 2π‘‰π‘ π‘–π‘›πœƒ
𝑅 = π»π‘œπ‘Ÿπ‘–π‘§π‘œπ‘›π‘‘π‘Žπ‘™ π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’(π‘Ÿπ‘Žπ‘›π‘”π‘’)
𝑔
𝑅 = π‘‰π‘π‘œπ‘ πœƒ ×
𝑅=
𝑣 2 𝑠𝑖𝑛2πœƒ
𝑔
2π‘£π‘ π‘–π‘›πœƒ
𝑔
=
𝑣 2 2π‘ π‘–π‘›πœƒπ‘π‘œπ‘ πœƒ
𝑔
(𝑠𝑖𝑛2πœƒ = 2π‘ π‘–π‘›πœƒπ‘π‘œπ‘ πœƒ)
π‘šπ‘Žπ‘₯. π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘ π‘–π‘›πœƒ = 1 π‘€β„Žπ‘’π‘› πœƒ = 90°
π‘‘β„Žπ‘’π‘Ÿπ‘’π‘“π‘œπ‘Ÿπ‘’ 2πœƒ = 90°
πœƒ = 45°
π‘‡β„Žπ‘’π‘Ÿπ‘’π‘“π‘œπ‘Ÿπ‘’ π‘šπ‘Žπ‘₯. 𝑅 𝑖𝑠 π‘€β„Žπ‘’π‘› πœƒ = 45 °
𝑣2
𝑅=
𝑔
𝑠𝑖𝑛𝑐𝑒 max π‘œπ‘“ sin 2πœƒ = 1
V
πœƒ
Vcosπœƒ
2 Angles of projection for all other ranges other than max range
𝑣 2 𝑠𝑖𝑛2πœƒ
𝑅=
𝑔
𝑅𝑔
𝑠𝑖𝑛2πœƒ = 2
𝑣
−1 𝑅𝑔
sin
𝑣2
πœƒ=
2
Parabolic path of projectile
Vertical Analysis
1
𝑠 = 𝑒𝑑 + π‘Žπ‘‘ 2
2
1
𝑦 = π‘‰π‘£π‘’π‘Ÿπ‘‘ 𝑑 + 2 (−9.8)𝑑 2
y = vertical distance
Horizontal Analysis
π‘₯
π‘‰β„Žπ‘œπ‘Ÿπ‘– =
𝑑
π‘₯
𝑑=
π‘‰β„Žπ‘œπ‘Ÿπ‘–
Therefore 𝑦 =
π‘‰π‘£π‘’π‘Ÿπ‘‘ π‘₯
π‘‰β„Žπ‘œπ‘Ÿπ‘–
π‘₯ = β„Žπ‘œπ‘Ÿπ‘–π‘§π‘œπ‘›π‘‘π‘Žπ‘™ π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’
–
4.9
2
π‘‰β„Žπ‘œπ‘Ÿπ‘–
π‘₯2
Therefore path is parabolic (only for short distances due to curvature of earth surface)
Space
Important Values
G = gravitational constant 6.67 × 10−11
Radius of earth = 6.4 × 106 π‘š
Mass of earth = 5.9742 × 1024 kilograms
“G force”
π‘Žπ‘π‘π‘Žπ‘Ÿπ‘’π‘›π‘‘ π‘€π‘’π‘–π‘”β„Žπ‘‘ π‘š(𝑔 + π‘Ž) 𝑔 + π‘Ž
“𝑔” =
=
=
π‘Žπ‘π‘‘π‘’π‘Žπ‘™ π‘€π‘’π‘–π‘”β„Žπ‘‘
π‘šπ‘”
𝑔
Example 2: 65kg physics student shot out of a cannon in a lift and is falling back to earth
g=
π‘š(𝑔+π‘Ž)
π‘šπ‘”
=
π‘š(9.8+ −9.8)
π‘šπ‘”
=0
Example 3: 65kg physics student goes on circular rollercoaster loop and is upside travelling 15m/s what is
his apparent weight
15m/s
11.25m/s/s acceleration due to loop
Radius = 20m
9.8ms/s/s gravity
g = 9.8m/s/s
π‘Ž=
𝑣2
π‘Ÿ
=
152
20
= 11.25m/s/s
π‘Žπ‘’π‘“π‘“ = 11.25 – 9.8 = 1.45m/s/s
F = ma
= 65
1.45
=94.25N
Circular motion
Orbital velocity = v
Centripetal force, 𝐹𝑐 =
π‘šπ‘£ 2
π‘Ÿ
Centripetal acceleration/ acceleration of circular motion =
𝑣2
π‘Ÿ
Escape velocity = speed of launch so that the speed when the object is a very large distance away is zero
(relative to earth/ object launched from)
Rockets
Balloon (similar of like rocket combustion chamber)
Air Particles
Zero Net force
Net forward push
The removal of a force from a previously balanced system >>> net force >>> acceleration
The force of air particles impacting on front end of balloon causes balloon to be propelled forward
Combustion chamber
Exhaust
Fuel
Oxygen
Exhaust particles impact on front end of combustion chamber propelling rocket forward
Due to conservation of momentumβˆ†π‘š × π‘‰π‘’π‘₯β„Žπ‘Žπ‘’π‘ π‘‘ = 𝑀 × βˆ†π‘‰π‘Ÿπ‘œπ‘π‘˜π‘’π‘‘
πΉπ‘Ÿπ‘’π‘ 
π‘Ž=
π‘š
βˆ†π‘ π‘šπ‘£ − π‘šπ‘’
πΉπ‘Ÿπ‘’π‘  =
=
βˆ†π‘‘
𝑑
πΉπ‘Ÿπ‘’π‘  × π‘‘ = π‘šπ‘£ − π‘šπ‘’
Thrust of Rocket = rate of change of momentum of rocket
βˆ†π‘
=
π‘œπ‘“ π‘Ÿπ‘œπ‘π‘˜π‘’π‘‘
βˆ†π‘‘
=
π‘€βˆ†π‘£
βˆ†π‘‘
βˆ†π‘€π‘£π‘’
=
( βˆ†π‘š × π‘‰π‘’π‘₯β„Žπ‘Žπ‘’π‘ π‘‘ = 𝑀 × βˆ†π‘‰π‘Ÿπ‘œπ‘π‘˜π‘’π‘‘ )
βˆ†π‘€
= 𝑣𝑒
βˆ†π‘‘
βˆ†π‘š
βˆ†π‘€
But = −
βˆ†π‘‘
βˆ†π‘‘
βˆ†π‘‘
Therefore thrust on rocket =
βˆ†π‘€
βˆ†π‘‘
= 𝑣𝑒
Force of Gravity
πΉπ‘”π‘Ÿπ‘Žπ‘£ =
πΊπ‘€π‘š
d = distance from centre of 1st mass to centre of 2nd mass
𝑑2
Acceleration due to gravity
π‘Ž=
𝑓
π‘š
π‘Žπ‘” =
𝑔=
πΊπ‘€π‘š
𝑑2
π‘š
𝐺𝑀
𝑔 = π‘Žπ‘π‘π‘’π‘™π‘’π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘› 𝑑𝑒𝑒 π‘‘π‘œ π‘”π‘Ÿπ‘Žπ‘£π‘–π‘‘π‘¦
𝑑2
Orbital Velocity of Satellite
𝐺𝑀
π‘Žπ‘” =
𝑑2
𝑣2
π‘Ž=
𝑑
2
𝑣
𝐺𝑀
= 2
𝑑
𝑑
𝑣2 =
𝐺𝑀
𝑑
𝐺𝑀
𝑣= √
𝑑
𝑏𝑒𝑑 𝑣 =
2
𝑣 =
>>>>> Orbital Velocity of Satellite
2πœ‹π‘‘
𝑃
4πœ‹2 𝑑2
𝑃2
2 2
∴
4πœ‹ 𝑑
𝐺𝑀
=
2
𝑃
𝑑
4πœ‹2
𝑃2 = (
𝐺𝑀
) 𝑑 3 >>>>>>Orbital period formula
Low earth orbit
250km – 1000km high enough to avoid atmospheric drag while avoiding Van Allen radiation belt
Geostationary Orbit
An orbit at an altitude at which the period of the satellite’s orbit = period of orbit of earth (1 sidereal day
3mins 56 secs shorter than 24 hour day)
If this orbit is over the equator the satellite would remain ‘parked’ over a fixed point on the earth’s surface.
Useful for comm. Sat. as a receiving dish will only need to point in one direction.
The radius of the orbit is calculated using Kepler’s law of periods and = 42 167 km (approx. 35800 above
earth surface)
Effect of the Earth’s motion on a launch
To increase efficiency, reduce fuel consumption etc. Orbits of the earth other planets can be used to
increase the speed of satellites/rockets etc.
1.
Earth surface rotates at 1700km/h relative to sun and orbits it at 10700km/h – rockets are launched
to the east to give them a boost – timed to give maximum boost in desired direction
2.
Slingshot effect – a space probe is given a boost as it passes by and is pulled in by the planet’s
gravitational effect; it acquires the speed of the planet relative to the sun
Effective
velocity
Planet
Motion of
planet
Probe travelling
past planet
Elliptical Orbits
Most orbits are elliptical
Gravitational Potential energy of orbiting Satellite
𝑬𝒑 = GPE = Energy of mass due to its position within a gravitational field.
𝐺𝑃𝐸 = π‘šπ‘”β„Ž
π‘š = π‘šπ‘Žπ‘ π‘  𝑔 = 9.8 β„Ž = β„Žπ‘’π‘–π‘”β„Žπ‘‘
In falling objects
KE gained = grav. PE lost
1
π‘šπ‘£ 2 = π‘šπ‘”β„Ž
2
π‘šπ‘£ 2 = 2π‘šπ‘”β„Ž
𝑣 2 = 2π‘”β„Ž
𝑣 = √2π‘”β„Ž >>>> final velocity of falling object prior hitting ground
The zero reference point of GPE is
distance away because Fgrav = 0 at
Work must be done to move objects altitude away from earth
distance
Therefore
GPE at
=0
Therefore at point near earth GPE < 0
Mathematical derived >>> 𝐺𝑃𝐸 = −𝐺
Mm
𝑑
M = mass of planet; m = mass of object ; d =
distance seperating masses (m)
π‘šπ‘”β„Ž = π‘šπ‘” × β„Ž
=𝐹 ×𝑑
= π‘€π‘œπ‘Ÿπ‘˜ π‘‘π‘œπ‘›π‘’
πΊπ‘€π‘š
πΊπ‘€π‘š
πΊπ‘€π‘š
π‘€π‘œπ‘Ÿπ‘˜ =
× βˆ†π‘‘ + … ..
2 × βˆ†π‘‘ +
2 × βˆ†π‘‘ +
𝑑1
𝑑2
𝑑32
=∑
πΊπ‘€π‘š
𝑑2
=∫
× βˆ†π‘‘
πΊπ‘€π‘š
× βˆ†π‘‘
𝑑2
Kinetic energy of orbiting satellite
𝐾𝐸 =
1
π‘šπ‘£ 2
2
πΎπΈπ‘œπ‘Ÿπ‘π‘–π‘‘π‘–π‘›π‘” π‘ π‘Žπ‘‘π‘’π‘™π‘™π‘–π‘‘π‘’ =
1 πΊπ‘€π‘š
×
2
𝑑
π‘Žπ‘ 
π‘£π‘œπ‘Ÿπ‘π‘–π‘‘ = √
𝐺𝑀
𝑑
πΎπΈπ‘œπ‘Ÿπ‘π‘–π‘‘π‘–π‘›π‘” π‘ π‘Žπ‘‘π‘’π‘™π‘™π‘–π‘‘π‘’ =
πΊπ‘€π‘š
2𝑑
Total energy of orbiting satellite
Total energy =
= −
πΊπ‘€π‘š
2𝑑
−𝐺
Mm
𝑑
1 πΊπ‘€π‘š
2
𝑑
Therefore for escape velocity
(π‘™π‘Žπ‘’π‘β„Ž)
1
πΊπ‘€π‘š
π‘šπ‘£π‘’π‘ π‘π‘Žπ‘π‘’ 2 −
= 0 + 0 (Energy at very large distance away)
2
𝑑
1
πΊπ‘€π‘š
π‘šπ‘£π‘’π‘ π‘π‘Žπ‘π‘’ 2 =
2
𝑑
π‘£π‘’π‘ π‘π‘Žπ‘π‘’ 2 =
π‘£π‘’π‘ π‘π‘Žπ‘π‘’
2𝐺𝑀
𝑑
=√
2𝐺𝑀
𝑑
Changing Satellite orbits
Total final energy (KE + GPE) = total initial energy (KE + GPE) + energy provided by fuel
𝐾𝐸𝑓𝑒𝑒𝑙 = πΉπ‘–π‘›π‘Žπ‘™ π‘‘π‘œπ‘‘π‘Žπ‘™ π‘’π‘›π‘’π‘Ÿπ‘”π‘¦ − π‘–π‘›π‘–π‘‘π‘Žπ‘™ π‘‘π‘œπ‘‘π‘Žπ‘™
Example: Raising satellite from 300km to 500km orbit above earth using 141kJ/gram hydrogen fuel
−
1
πΊπ‘€π‘š
2
6.9 ×106
= −
1
πΊπ‘€π‘š
2 6.7 ×106
+ 141 × 103 × βˆ†π‘šβ„Žπ‘¦π‘‘π‘Ÿπ‘œπ‘”π‘’π‘›
Magnetism
Characteristics of Magnets
1.
Like poles repel (N and N, S and S)
2.
Unlike poles attract (N and S)
3.
Strongly Magnetic metals (metals greatly affected by magnets) are Iron, Nickel and Cobalt. These can be
made into magnets. Other metals are only slightly magnetic
4.
Magnetically effected metals become Induced Magnetic Dipoles in a magnetic field therefore they are
attracted by the magnet. Magnetic metals align to the magnetic “field lines” of a magnet
5.
Direction of “magnetic” flow is from north to south on a magnet
6.
Strength of Magnetic field is measured in Teslas (T)
7.
Earth act’s like a giant magnets and compasses point north as they align with magnetic feild
8.
S magnetic pole is near north pole, N magnetic pole is near south pole N end of magnet points near north
andS end of magnet points close to south
9.
Magnetic field of earth flips every few million years – evidence in solidified lava containing magnetic
minerals surrounding volcanoes
10.
All Magnetic fields are created by moving charges, Wires have magnetic field with no N and S
Important Conventions
Right hand thumb rule
Thumb points in
Direction of current
Fingers curl in
direction of
magnetic field
Right Hand Force rule
Fingers in direction of
magnetic field
Thumb pointing
direction of
current in wire
Palm “pushes” in
direction of resulting
force
Right hand push rule – for generators
Fingers in direction of
magnetic field
Movement of
positive charge
in wire
Direction of force on
positive charge in wire
i.e. direction of induced
current
3D drawing conventions
Direction: Out of page
– Arrow head shot
through page from
behind
Direction: Into Page –
Arrow shot into page
feathers showing on
back of arrow
Magnets in Detail
Inside magnets the magnetic field flows from S to N , outside the field flows from N to S. Forming “loops”
Magnetism Terminology
Faraday Called this “Magnetic Fluid” / “Magnetic Flux” symbol = ∅
𝐡 = π»π‘œπ‘€ π‘šπ‘’π‘β„Ž "magnetic flow" per square meter
= π‘Šπ‘’π‘π‘’π‘Ÿπ‘ /π‘š2
∅
=
𝐴
= 𝑇 ("π‘‡π‘’π‘ π‘™π‘Žπ‘ ")
Solenoids
A Solenoid is a coil of conducting wire rolled into a helical spiral.
Characteristics
They generate magnetic fields with a north and south pole.
The magnetic field inside is relatively uniform
π‘šπ‘’π‘Žπ‘ π‘’π‘Ÿπ‘’π‘‘ 𝑖𝑛 π‘€π‘’π‘π‘’π‘Ÿπ‘  π‘Šπ‘
Electric Motors
Magnetics interact with the magnetic field generated by a solenoid causes the motor to turn
Efficiency of a motor is improved by using multiple coils – which increases the time which magnetic force acts to
rotate shaft.
Using magnets with rounded ends to create pseudo radial pattern – changes the direction of force so that it acts
more at a tangent to the circular path of the coil which increases the effective force on the rotation.
Commutator
Mechanical switch used the current every half revolution so the coil keeps rotating in a constant direction.
Shaft
The solenoid, Commutator are attached to the shaft and is used to transfer the kinetic energy so it can do work.
The Commutator and solenoid are aligned so the gap between the two halves of the Commutator is perpendicular to
the solenoid.
Ammeter
A motor with no Commutator and spring attached to shaft
Magnetic force of 2 wires
𝐼1 𝐼2 𝑙
πΉπ‘šπ‘Žπ‘” ∝
𝑑
πΉπ‘šπ‘Žπ‘”
𝐼1 𝐼2
=𝐾
𝐾 = 2 × 10−7 (π΄π‘šπ‘π‘’π‘Ÿπ‘’π‘  πΆπ‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘ ) ; 𝑙
𝑙
𝑑
= π‘™π‘’π‘›π‘”π‘‘β„Ž π‘œπ‘“ π‘€π‘–π‘Ÿπ‘’ (π‘™π‘’π‘›π‘”π‘‘β„Ž π‘œπ‘“ π‘ π‘’π‘π‘‘π‘–π‘œπ‘›π‘  π‘π‘Žπ‘Ÿπ‘Ÿπ‘Žπ‘™π‘™π‘’π‘™) ; 𝑑 = π‘‘π‘–π‘ π‘‘π‘›π‘Žπ‘π‘’ 𝑏𝑒𝑑𝑀𝑒𝑒𝑛 π‘€π‘–π‘Ÿπ‘’π‘ 
Amperes constant ‘K’ was defined and not experimentally determined – Used to determine 1 amp
NOTE: If the two wires that are parallel are different in length the shorter length is taken – this is because the section
of wire that has no wire parallel to it does not experience a magnetic force as the magnetic field of that section of
wire does not interact with other magnetic fields.
A current carrying wire only experiences a magnetic force when the magnetic field is perpendicular to the wire.
Strength of Magnetic Field
πΉπ‘šπ‘Žπ‘” ∝ 𝐡 ; πΉπ‘šπ‘Žπ‘” ∝ 𝑖 (π‘π‘’π‘Ÿπ‘Ÿπ‘’π‘›π‘‘ 𝑖𝑛 π‘€π‘–π‘Ÿπ‘’); πΉπ‘šπ‘Žπ‘” ∝ 𝑙 (length of wire)
πΉπ‘šπ‘Žπ‘” = 𝐡𝑖𝑙
πΉπ‘šπ‘Žπ‘”
𝐡=
𝑖𝑙
𝐡 = π‘€π‘Žπ‘”π‘›π‘’π‘‘π‘–π‘ 𝑓𝑒𝑖𝑙𝑑 π‘ π‘‘π‘Ÿπ‘’π‘›π‘”π‘‘β„Ž π‘šπ‘’π‘Žπ‘ π‘Ÿπ‘’π‘’π‘‘ 𝑖𝑛 π‘‡π‘’π‘ π‘™π‘Žπ‘  (𝑇)
𝐼
𝐡 = 𝐾 𝑑1 For around a current carryin gwires
When wire is not perpendicular to magnetic field
πΉπ‘šπ‘Žπ‘” = 𝐡𝑖𝑙 π‘ π‘–π‘›πœƒ
βƒ—
π‘Šβ„Žπ‘’π‘Ÿπ‘’ πœƒ = π‘Žπ‘›π‘”π‘™π‘’ 𝑏𝑒𝑑𝑀𝑒𝑒𝑛 𝐼 π‘Žπ‘›π‘‘ 𝐡
Generators
Conv. I
Fmag
I
e
V
e
e
e
e
e
e
e
e
Lenz’s Law
An induced current will produce a magnetic field which will interact with the
external magnetic field to produce a magnetic force opposing the change which
caused it.
I
Fmag
V
Principle can be used to determine the current in wires moving through magnetic fields etc. by using right hand force
rule with force in opp direction of movement.
Generator Formulas
πΉπ‘šπ‘Žπ‘” = π‘žπ‘£π΅
π‘ž = π‘β„Žπ‘Žπ‘Ÿπ‘”π‘’ 𝑣 = 𝑠𝑝𝑒𝑒𝑑
≫ πΉπ‘šπ‘Žπ‘” = 𝐡𝑖𝑙 𝑖𝑛 𝑑𝑖𝑠𝑔𝑒𝑖𝑠𝑒
π‘€π‘œπ‘Ÿπ‘˜ π‘‘π‘œπ‘›π‘’ π‘‘π‘œ π‘šπ‘œπ‘£π‘’ π‘ž π‘“π‘Ÿπ‘œπ‘š 1 𝑒𝑛𝑑 π‘œπ‘“ π‘€π‘–π‘Ÿπ‘’ π‘‘π‘œ π‘Žπ‘›π‘œπ‘‘β„Žπ‘’π‘Ÿ = 𝐹 × π‘‘
= πΉπ‘šπ‘Žπ‘” × π‘™
π‘Š = π‘žπ‘£π‘ × π‘™
π‘€π‘œπ‘Ÿπ‘˜
π΅π‘Žπ‘‘π‘‘π‘’π‘Ÿπ‘¦ π‘π‘œπ‘™π‘‘π‘Žπ‘”π‘’ =
π‘π‘œπ‘’π‘™π‘œπ‘šπ‘
π‘žπ‘£π‘ × π‘™
=
π‘ž
= 𝑣𝑏𝑙
𝐸. 𝑀. 𝐹(π‘’π‘™π‘’π‘π‘‘π‘Ÿπ‘œπ‘šπ‘œπ‘‘π‘–π‘£π‘’ π‘“π‘œπ‘Ÿπ‘π‘’) = 𝑣𝐡𝑙 sin πœƒ
πΈπ‘šπ‘“ = 𝑣𝐡𝑙
𝑣𝐡𝑙 × π‘‘
=
𝑑
(𝑣𝑑 × π‘™ ) × π΅
=
𝑑
𝐴 ×𝐡
=
𝑑
𝐡𝐴
=
𝑑
∅
∅
=
π‘Žπ‘  𝐡 =
𝑑
𝐴
πœƒ = π‘Žπ‘›π‘”π‘™π‘’ 𝑏𝑒𝑑𝑀𝑒𝑒𝑛 𝑣 π‘Žπ‘›π‘‘ 𝐡
πΈπ‘šπ‘“ = −
βˆ†∅
βˆ†π‘‘
πΉπ‘Žπ‘Ÿπ‘Žπ‘‘π‘Žπ‘¦π‘  πΏπ‘Žπ‘€
Back emf
Every motor acts as a generator once in motion as it is a coil moving past magnet
This causes a current to be generated in the opposite direction of the supplied current hence name Back
emf.
𝑁𝑒𝑑 π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’ = 𝑉 − 𝑖𝑛𝑑𝑒𝑐𝑒𝑑 π‘π‘Žπ‘π‘˜ π‘’π‘šπ‘“
𝑖𝑛𝑑𝑒𝑐𝑒𝑑 𝐸𝑀𝐹 ≤ 𝑉
Effects:
1.
Controls spin rate
2.
Prevents motor burn out
3.
If motor jams > no back emf > huge current > damages motor > burns insulation
4.
Start up high current can burn motor > solution is variable resistor gradually opened
Transformers
Primary Coil = Input
Iron core = Flux linkage
Step down transformer
Voltage in primary coil is higher than voltage in secondary coil
Current in Secondary coil determines current in Primary
𝑉𝑠 𝑛𝑠
=
π‘“π‘œπ‘Ÿ π‘–π‘‘π‘’π‘Žπ‘™ π‘‘π‘Ÿπ‘Žπ‘›π‘ π‘“π‘œπ‘Ÿπ‘šπ‘’π‘Ÿπ‘ 
𝑉𝑝 𝑛𝑝
𝑃𝑝 = 𝑃𝑠
π‘“π‘œπ‘Ÿ π‘–π‘‘π‘’π‘Žπ‘™ π‘‘π‘Ÿπ‘Žπ‘›π‘ π‘“π‘œπ‘Ÿπ‘šπ‘’π‘Ÿπ‘ 
𝑉𝑝 𝐼𝑝 = 𝑉𝑠 𝐼𝑠
𝐼𝑠 𝑉𝑝 𝑛𝑝
= =
𝐼𝑝 𝑉𝑠 𝑛𝑠
Principle of Conservation of energy
𝑃𝑝 ≥ 𝑃𝑠
π‘“π‘œπ‘Ÿ π‘Ÿπ‘’π‘Žπ‘™ π‘‘π‘Ÿπ‘Žπ‘›π‘ π‘“π‘œπ‘Ÿπ‘šπ‘’π‘Ÿπ‘ 
𝑃𝑠 = 𝐸𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑐𝑦 𝑖𝑛 π‘π‘’π‘Ÿπ‘π‘’π‘›π‘‘π‘Žπ‘”π‘’ × π‘ƒπ‘
Electrical Distribution Networks
AC Generator Step up transformer
Transformers
High Voltage Transmission lines
Local Network
Power generated at 11000 V stepped up to 500 000V
High Voltage wires are insulated from poles using ceramic cups
1.
Cup shape to keep conducting rain off
Why do this?
1.
Especially with non-ideal transformers
Can Transmit same power at:
2.
High V, Low I
3.
Low V, High I (𝑃 = 𝑉𝐼)
Series of Step down
High V and low I preferred as:
1.
Decreases 𝐼 2 𝑅 Losses in transmission lines
π‘Š(π‘π‘œπ‘€π‘’π‘Ÿ π‘Žπ‘  β„Žπ‘’π‘Žπ‘‘ 𝑖𝑛 π‘€π‘–π‘Ÿπ‘’π‘ ) = 𝑉 × πΌ
𝑉2
=
𝑅
𝑉2𝑅
= 2
𝑅
= 𝐼2 𝑅
Series of Step down transformers for safety in suburban areas
Insulated Laminations
ο‚· Iron cores of transformers – made from thin sheets of metal sandwiched with thin insulation
ο‚· Reduces eddy currents
ο‚· Heat
ο‚· Power losses
ο‚· Small sheets result in smaller eddy currents
ο‚· Results in less power loss
3 phase power supply
3 generators in 1 – each coil connected to own set of slip rings – resulting in 3 currents
Torque – Twisting force (angular accerlation)
𝜏 = π‘‡π‘œπ‘Ÿπ‘žπ‘’π‘’ = 𝐹⊥ × π‘‘π‘“π‘Ÿπ‘œπ‘š π‘π‘–π‘£π‘œπ‘‘ π‘ˆπ‘›π‘–π‘‘π‘’π‘  = π‘π‘š (π‘π‘’π‘€π‘‘π‘œπ‘› π‘€π‘’π‘‘π‘’π‘Ÿπ‘ )
πœπ‘Ÿπ‘œπ‘‘π‘œπ‘Ÿπ‘π‘œπ‘–π‘™ = 𝑛𝐡𝐼𝐴 πΆπ‘œπ‘ πœƒ πœƒ = ∠𝑏𝑒𝑑𝑀𝑒𝑒𝑛 π‘π‘™π‘Žπ‘›π‘’ π‘œπ‘“ π‘™π‘œπ‘œπ‘ π‘Žπ‘›π‘‘ 𝐡 𝑓𝑖𝑒𝑙𝑑 𝑙𝑖𝑛𝑒𝑠
𝐴 = π‘Žπ‘Ÿπ‘’π‘Ž π‘œπ‘“ π‘π‘œπ‘–π‘™
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