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Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 0 q E dA What does it mean? How do we use it?

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Page 1: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

Gauss’s Law

Dominic BerryUniversity of Waterloo

Griffith University8 February, 2011

0

qE dA

What does it mean?

How do we use it?

Page 2: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

Area A

Page 3: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

E

Area A

Electric field

Page 4: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

E

Area A

Electric field

Flux is just electric field times area EA

Page 5: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

If electric field does not pass through the area, flux is zero.

0

E

Page 6: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

In general we use a normal vector to the plane, .

A

A

Page 7: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

For more general angles the flux varies as cos.

cosEA E A

AE

Page 8: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

First we need the concept of flux.

90

E

0

E

A

A

A

For more general angles the flux varies as cos.

cosEA E A

E

EA 0

cos 1 cos 0

Page 9: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

Page 10: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

We use the convention that the normal always points outward.

Page 11: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

E We use the convention that

the normal always points outward.

Page 12: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

E We use the convention that

the normal always points outward.

For the four sides, 0E A

Page 13: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

E We use the convention that

the normal always points outward.

For the four sides,

For the top,

0E A

E A EA

Page 14: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

E We use the convention that

the normal always points outward.

For the four sides,

For the top,

For the bottom,

0E A

E A EA

E A EA

Page 15: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The total flux through a closed surface.

E We use the convention that

the normal always points outward.

For the four sides,

For the top,

For the bottom,

The total flux is

0E A

E A EA

E A EA

0EA EA

Page 16: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

What does the integral mean?

E

The circle indicates an integral over the closed surface.

E dA

Page 17: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

What does the integral mean?

E E dA

The circle indicates an integral over the closed surface.

In practice we will not have to evaluate the interval.

Page 18: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

What does the integral mean?

E E dA

The circle indicates an integral over the closed surface.

In practice we will not have to evaluate the interval.

We break the surface up into sections where the flux is easy to calculate.

Page 19: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

What does the integral mean?

E E dA

The circle indicates an integral over the closed surface.

In practice we will not have to evaluate the interval.

We break the surface up into sections where the flux is easy to calculate.

dA

In principle sum over infinitesimal elements .dA

Page 20: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The full Gauss’s law.

E

The left side is the total flux out through the surface.

0

qE dA

Page 21: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The full Gauss’s law.

E

The left side is the total flux out through the surface.

The right side is proportional to the charge, q, inside the surface.

0

qE dA

+q

Page 22: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

What does it mean?

The full Gauss’s law.

E

The left side is the total flux out through the surface.

The right side is proportional to the charge, q, inside the surface.

The constant, 0, is the usual vacuum permittivity.

0

qE dA

+q

Page 23: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q.

+q

r

Page 24: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface.

+q

r

Page 25: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

E

E

E

E

E

+q

r

Page 26: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

E

E

E

E

E

+q

r

Page 27: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

The flux is just EA.

E

E

E

E

E

+q

r

Page 28: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

The flux is just EA. Gauss’s law gives

E

E

E

E

E

0

qEA

+q

r

Page 29: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

The flux is just EA. Gauss’s law gives

E

E

E

E

E

0

qEA

2

0

4q

E r

+q

r

Page 30: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it? For example, consider a charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

The flux is just EA. Gauss’s law gives

E

E

E

E

E

0

qEA

2

0

4q

E r

204

qE

r

+q

r

Page 31: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it?

E

E

E

E

E

0

qEA

2

0

4q

E r

204

qE

r

+q

Consider a shell of charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

The flux is just EA. Gauss’s law gives

r

Page 32: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it?

E

E

E

E

E

0

0EA

24 0E r

0E

+q

Consider a shell of charge q. We choose a spherical surface. By spherical symmetry the electric

field must be directed radially outwards.

The magnitude of the electric field must be constant on the surface.

The flux is just EA. Gauss’s law gives

r

Page 33: Gauss’s Law Dominic Berry University of Waterloo Griffith University 8 February, 2011 What does it mean? How do we use it?

How do we use it?

General procedure: Choose a surface corresponding

to the symmetry of the problem.

Break the surface up into subsurfaces where the electric field is either

1. constant and parallel to the normal, or

2. perpendicular to the normal.

Evaluate the total flux using the electric field as a free parameter.

Solve Gauss’s law for E.

E

E

E

E

E

r

+q

http://www.dominicberry.org/presentations/gauss.ppt