Calculus 3 introduction to cross product

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SUMMARY

The discussion focuses on the properties and definitions of the cross product in three-dimensional vector calculus. It clarifies that the cross product is not a resultant vector but is always orthogonal to the two vectors being multiplied. The magnitude of the cross product represents the area of the parallelogram formed by the two vectors, while the dot product measures how parallel the vectors are. Additionally, the relationship between the cosine of the dot product and the sine of the cross product is highlighted, emphasizing their respective roles in vector analysis.

PREREQUISITES
  • Understanding of three-dimensional vectors
  • Familiarity with vector operations: cross product and dot product
  • Knowledge of geometric interpretations of vectors
  • Basic grasp of trigonometric functions related to angles
NEXT STEPS
  • Study the geometric interpretation of the cross product in vector calculus
  • Learn about the properties of the dot product and its applications
  • Explore the Jacobi identity and its significance in vector operations
  • Investigate the relationship between vector angles and trigonometric functions
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Students and educators in mathematics, physics, and engineering, particularly those focusing on vector calculus and its applications in three-dimensional space.

lonewolf219
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Just learning about vectors in 3 dimensions. Would it be correct to think of the cross product vector like a resultant vector? Is it similar to the displacement? If so, why is it always 90 degrees from both original vectors?

If anyone has some deeper insight into any of these vector topics I would appreciate it. Also, I'm wondering what the dot product is actually measuring. And what the relationship is beteen the cosine of dot product and the sine of cross product...

THANK YOU!
 
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lonewolf219 said:
Just learning about vectors in 3 dimensions. Would it be correct to think of the cross product vector like a resultant vector? Is it similar to the displacement? If so, why is it always 90 degrees from both original vectors?

If anyone has some deeper insight into any of these vector topics I would appreciate it. Also, I'm wondering what the dot product is actually measuring. And what the relationship is beteen the cosine of dot product and the sine of cross product...

THANK YOU!

In order...

No, the cross product is not a resultant vector, at least not as I understand the term. As I understand it, the resultant vector is a sum of two other vectors. Or more.

I'm not sure if it'd be similar to the displacement, myself. That depends on what you mean by displacement.

The cross product is always orthogonal to the two vectors being cross producted because that's how it's defined. As for what they're measuring...

The magnitude of the cross product can be thought of as measuring the area of the parallelogram defined by its two component vectors. Picture below:

220px-Cross_product_parallelogram.svg.png


As you can see, the cross product vector itself will always be orthogonal to that parallelogram.
 
Another way to define the cross product is to define
1) \vec{i}\times\vec{j}= \vec{k}
2) \vec{j}\times\vec{k}= \vec{i}
3) \vec{k}\times\vec{i}= \vec{k}

and defining it to be associative, distributive, and anti-commutative so
that (a\vec{i}+ b\vec{j}+ c\vec{k})\times(u\vec{i}+ v\vec{j}+ w\vec{k})= a\vec{i}\times(u\vec{i}+ v\vec{j}+ w\vec{k})+ b\vec{j}\times(u\vec{i}+ v\vec{j}+ w\vec{k})+ c\vec{k}(u\vec{i}+ v\vec{j}+ w\vec{k})
 
Another way to think about it is that, while the (absolute value of the) dot product tells you "how parallel" two vectors are, the (magnitude of the) cross product tells you "how perpendicular" two vectors are.
 
Thanks for the replies, guys! Hmm, the angle of how parallel and the angle of how perpendicular. That's interesting!
 
HallsofIvy said:
Another way to define the cross product is to define
1) \vec{i}\times\vec{j}= \vec{k}
2) \vec{j}\times\vec{k}= \vec{i}
3) \vec{k}\times\vec{i}= \vec{k}

and defining it to be [strike]associative[/strike], distributive, and anti-commutative so
that (a\vec{i}+ b\vec{j}+ c\vec{k})\times(u\vec{i}+ v\vec{j}+ w\vec{k})= a\vec{i}\times(u\vec{i}+ v\vec{j}+ w\vec{k})+ b\vec{j}\times(u\vec{i}+ v\vec{j}+ w\vec{k})+ c\vec{k}(u\vec{i}+ v\vec{j}+ w\vec{k})
There's one word too many in that sentence. The cross product isn't associative. It satisfies the Jacobi identity instead: a×(b×c)+b×(c×a)+c×(a×b)=0.
 
Relativistic Momentum, Mass, and Energy Momentum and mass (...), the classic equations for conserving momentum and energy are not adequate for the analysis of high-speed collisions. (...) The momentum of a particle moving with velocity ##v## is given by $$p=\cfrac{mv}{\sqrt{1-(v^2/c^2)}}\qquad{R-10}$$ ENERGY In relativistic mechanics, as in classic mechanics, the net force on a particle is equal to the time rate of change of the momentum of the particle. Considering one-dimensional...

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