Media Summary: ... parameterized and explicit representations then uh ... all that any vector field can be decomposed into ... a cylindrical case on the left hand side we ended up with this being equal to

Mat291 Tutorial 2 - Detailed Analysis & Overview

... parameterized and explicit representations then uh ... all that any vector field can be decomposed into ... a cylindrical case on the left hand side we ended up with this being equal to Plus one so so you see denominator is not zero so we get one over this is also square root of All to the power of p i can rewrite it as x squared plus y squared plus z squared to the power of p over

Photo Gallery

MAT291 Tutorial 2
MAT291 Lecture 2A
MAT291 Lecture 2B
MAT291 Review 2A
MAT291 Review 2B
MAT291 Review 2B
MAT291 Lecture 2C
MAT291 Lecture 2C
MAT291 Tutorial 1
MAT291 Tutorial 5
MAT291 Tutorial 0
MAT291 Tutorial 3
View Detailed Profile
MAT291 Tutorial 2

MAT291 Tutorial 2

So it would be plus or minus pi over

MAT291 Lecture 2A

MAT291 Lecture 2A

All right so now we need to introduce

MAT291 Lecture 2B

MAT291 Lecture 2B

Welcome to uh lecture

MAT291 Review 2A

MAT291 Review 2A

... parameterized and explicit representations then uh

MAT291 Review 2B

MAT291 Review 2B

... all that any vector field can be decomposed into

MAT291 Review 2B

MAT291 Review 2B

... a cylindrical case on the left hand side we ended up with this being equal to

MAT291 Lecture 2C

MAT291 Lecture 2C

... between 0 and

MAT291 Lecture 2C

MAT291 Lecture 2C

... zero and U would range between 0 and

MAT291 Tutorial 1

MAT291 Tutorial 1

Plus one so so you see denominator is not zero so we get one over this is also square root of

MAT291 Tutorial 5

MAT291 Tutorial 5

I evaluated the first integral and got

MAT291 Tutorial 0

MAT291 Tutorial 0

And this would be x minus

MAT291 Tutorial 3

MAT291 Tutorial 3

Which is going to be equal to

MAT291 Tutorial 6

MAT291 Tutorial 6

All to the power of p i can rewrite it as x squared plus y squared plus z squared to the power of p over