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Topic 6: Fields and forces State Newton’s universal law of gravitation. Students should be aware that the masses in the force law are point masses. The force between two spherical masses whose separation is large compared to their radii is the same as if the two spheres were point masses with their masses concentrated at the centers of the spheres. 6.1 Gravitational force and field

Topic 6: Fields and forces

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Topic 6: Fields and forces. 6.1 Gravitational force and field. Students should be aware that the masses in the force law are point masses. The force between two spherical masses whose separation is large compared to their radii is the same as if the two spheres were point masses with their - PowerPoint PPT Presentation

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Page 1: Topic 6: Fields and forces

Topic 6: Fields and forces

State Newton’s universal law ofgravitation.

Students should be aware that themasses in the force law are pointmasses. The force between twospherical masses whose separationis large compared to their radiiis the same as if the two sphereswere point masses with theirmasses concentrated at the centersof the spheres.

6.1 Gravitational force and field

Page 2: Topic 6: Fields and forces

Newton 1642-1727

Newton’s laws of gravitationAnything with mass attracts

anything else with mass. The size of that attraction is given

by my Law of Gravitation:

F = Gm1m2

r2

…where m1 and m2 are the masses of the two objects (in kg), r is the distance between them (in m) and G is “The Universal Gravitational Constant” (= 6.67 x 10-11 Nm2kg-2).

State Newton’s universal law ofgravitation.

Page 3: Topic 6: Fields and forces

Cavendish measurement of GClick to play

Page 4: Topic 6: Fields and forces
Page 5: Topic 6: Fields and forces

Inverse square law

Page 6: Topic 6: Fields and forces

What holds the planet in orbit?

Page 7: Topic 6: Fields and forces

Free Body Force Diagrams revision

The Earth attracts the man and the man attracts the Earth – a Newton III pair of forces where both are gravitational.

Page 8: Topic 6: Fields and forces

A uniform gravitational field is one where the field lines are always the same distance apart - this is almost exactly true close to the Earth's surface (Figure 1(a)).

However if we move back and look at the planet from a distance the field lines clearly radiate outwards (Figure 1(b)), getting further apart as the distance from the Earth increases.

When viewed from an even greater distance the complete field can be seen (Figure 1(c)).

Such a field is called a radial field - the field intensity (g) decreasing with distance.

Diagram 1(d) shows the distortion of the gravitational field lines by high- density rock.

Page 9: Topic 6: Fields and forces

Gravitational Field Strength

Consider a man on the Earth:

Man’s weight = mgBUT we know that this is equal to his gravitational attraction, so…

GMm = mg

r2

GM = g

r2

Therefore:

(this is a vector quantity)

Derive an expression for gravitational field strength at the surface of a planet, assuming that all its mass is concentrated at itscentre.

Page 10: Topic 6: Fields and forces

Gravitational Field StrengthDefine gravitational field strength.

Definition: Force, act, point, unit mass.

Write a definition of gravitational field strength

Determine the gravitational fielddue to one or more point masses.

Derive an expression for gravitational field strength at the surface of a planet, assuming that all its mass is concentrated at itscentre.

Page 11: Topic 6: Fields and forces

6.2 Electric force and fieldState that there are two types ofelectric charge.

Page 12: Topic 6: Fields and forces

Static Electricity

++

+ --

-

--

---

-

Page 13: Topic 6: Fields and forces

Conservation of charge

The law of conservation of charge states…………….

One of the fundamental laws of Physics is that charge can never be created or destroyed. Charge is always conserved in any reaction. A simple example of this is the rubbing of a polythene strip with a duster. Initially the strip and the dusted were uncharged but after rubbing the strip gains a net negative charge and the duster gains an equal amount of positive charge – the total charge in the process has been conserved.

State and apply the law ofconservation of charge.

Page 14: Topic 6: Fields and forces

Conductors and insulators.Describe and explain thedifference in the electricalproperties of conductors andinsulators.

In a conductor, the conduction and valence bands overlap. This allows the valence electrons to easily move along the conduction band giving the material low electrical resistance.

In insulators, there is a large forbidden energy band, which makes it difficult for valence electrons to move into the conduction band giving the material a high electrical resistance.

In semiconductors, the forbidden energy band is not too wide. Under certain conditions, electrons in the valence band can gain sufficient energy to cross the gap. This reduces the electrical resistance of the material.

The difference between conductors and insulators is………………

Page 15: Topic 6: Fields and forces

Coulomb’s lawState Coulomb’s law. Students should be aware that the charges

in the force law are point charges.

Page 16: Topic 6: Fields and forces

Coulomb’s Law

Charles Coulomb 1736-

1806

Like gravity, electrostatic force is one of the four fundamental forces. The equation

looks pretty similar too…

Coulomb’s Law

F = kQ1Q2

r2

…where k = 9.0 x 109 Nm2C-2 (the “Coulomb Law Constant”).This comes from k = 1/4πε0 …

…where ε0 = permittivity of free space (i.e. 8.85 x 10-12 Fm-1).

Page 17: Topic 6: Fields and forces

Electric field of a point chargeDefine electric field strength.

Write a definition of electric field strength

Students should understand theconcept of a test charge.

Determine the electric fieldstrength due to one or morepoint charges.

Page 18: Topic 6: Fields and forces

Electric field patterns

Draw the electric field patterns for different charge configurations.

These include the fields due to thefollowing charge configurations:a point charge, a charged sphere,two point charges, and oppositelycharged parallel plates. The latterincludes the edge effect. Studentsshould understand what is meantby radial field.

Page 19: Topic 6: Fields and forces

How do we predict the shape of a field?

• Imagine that you have a unit positive test charge.

• Place it in a point in the field.• Sketch the path it would take.• Repeat this many times until you have

enough field lines• The “density” of the lines represents the

strength of the field.

Page 20: Topic 6: Fields and forces

Point charge

+

Page 21: Topic 6: Fields and forces

Sphere

Positive or negative

Page 22: Topic 6: Fields and forces

2 Point charges

+ +

Page 23: Topic 6: Fields and forces

2 Point charges

+ -

Page 24: Topic 6: Fields and forces

Parallel plates

+

_

Edge effects

Page 25: Topic 6: Fields and forces

Electric FieldsElectric field strength E = F

q

(this is a bit like gravitional field strength g = F/m)

Let’s compare this to Coulomb’s Law:

Coulomb’s Law

F = kQq

r2

Putting these equations together gives us…

Electric field strength E = kQ

(in NC-1) r2

Page 26: Topic 6: Fields and forces

Electrostatic force and circular motionConsider an electron orbiting a nucleus in a hydrogen atom:

p

eQ. If the mass of an electron is 9.1x10-31kg and the distance to the proton is 0.11nm how fast is

the electron going?

Using mv2 = kQq we get v = 1.5x106 ms-1

r r2

Page 27: Topic 6: Fields and forces

A practical exampleConsider a charged polythene strip and a metal ball:

+

+ +

+--

--

- -- -

- -- -

-

Page 28: Topic 6: Fields and forces

Fields applet

Page 29: Topic 6: Fields and forces

Field for a point charge

Click to play

Page 30: Topic 6: Fields and forces

Electric dipoleClick to play

Page 32: Topic 6: Fields and forces

Electric fields around a point charge

Draw the edge effects for the parallel plate

2 Charged Spheres

http://www.falstad.com/emstatic/

Page 33: Topic 6: Fields and forces
Page 34: Topic 6: Fields and forces

Uniform electric fieldsConsider two charged plates:

+

-

Now consider a point charge:

QV

Work done = QV

For an electron, eV = ½mv2

Page 36: Topic 6: Fields and forces

6.3 Magnetic force and field

Page 37: Topic 6: Fields and forces

Permanent magnets and domains

Page 38: Topic 6: Fields and forces

HyperlinkState that moving charges give rise to magnetic fields.

Draw magnetic field patterns due to currents.

These include the fields due to currents in a straight wire, a flat circular coil and a solenoid.

Page 39: Topic 6: Fields and forces

Field around a wire

Click to play

Page 40: Topic 6: Fields and forces

Field around a loopClick to play

Page 41: Topic 6: Fields and forces

B field for a loop

Click to play

Page 42: Topic 6: Fields and forces

Field patterns

Page 43: Topic 6: Fields and forces

Left hand Motor RuleDetermine the direction of the forceon a current-carrying conductor in amagnetic field.

Page 44: Topic 6: Fields and forces

Fleming's left- hand rule

Page 45: Topic 6: Fields and forces

Current-carrying wire in a magnetic field

S

N

F = Force

B = Magnetic

field

I = Current

Q. Where will this wire go?

Page 46: Topic 6: Fields and forces

Comparing magnets and solenoids

N S

Magnet:

Solenoid:

Page 47: Topic 6: Fields and forces

Magnetic Field around a Solenoid

Page 48: Topic 6: Fields and forces

Forces on a loop

Click to play

Page 49: Topic 6: Fields and forces

Electric motor

Click to play

Page 51: Topic 6: Fields and forces

Magnetic Flux DensityClearly, the size of the force on this wire depends on three

things:

1. The strength of the magnetic field

2. The current in the wire

3. The length of the wire (in the field)

These three things are related by the simple formula…

B is called “magnetic flux density” and is measured in Teslas (= 1NA-1m-1). By definition, a magnetic flux density of 1T produces a force of 1N on a 1m long wire with a current of 1A.

Page 52: Topic 6: Fields and forces

Determine the direction of the force ona charge moving in a magnetic field.

Hamper HL page 208 Q’s 37,38 SL Page 141 Q’s 8,9.

Page 53: Topic 6: Fields and forces

Force on a charged particle

Page 54: Topic 6: Fields and forces

Define the magnitude and direction ofa magnetic field.

A magnetic flux density of 1T produces a force of 1N on a 1m long wire with a current of 1A.

Page 55: Topic 6: Fields and forces

Circular pathsRecall:

++

-2 protons, 2 neutrons, therefore charge =

+2

1 electron, therefore charge = -1

Because of this charge, they will be deflected by magnetic fields:

+

These paths are circular, so Bqv = mv2/r, orr =mv

Bq

Page 56: Topic 6: Fields and forces

Circular paths

if angle = 90° the path is circular

if 0 < angle < 90° the path is a helix.How do you work out which bit is circular?