Matrix transformations and effects on the unit square

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The discussion focuses on understanding the area transformation of the unit square under a matrix transformation T induced by matrix A, which is determined by the absolute value of the determinant of A, abs(det(A)). The transformation of unit vectors i and j into vectors Ti and Tj is examined, highlighting that the area of the parallelogram formed by these vectors can be calculated using the vector product without needing the sine of the angle between them, as they are unit vectors. The conversation also touches on the vector cross product's directionality and its dependence on the angles between the vectors involved. Additionally, it notes that while the magnitude of the area can be derived from the sine of the angle and the magnitudes of the vectors, the vector product simplifies this calculation. The discussion concludes by acknowledging the complexity of area transformations in higher dimensions.
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I was looking over my notes today, and I realized that there was a point that isn't pretty clear.

If we have the image under T (being T a matrix transformation induced by a matrix A) of the unit square, then its area should be abs(det(A)). Why is this though? I was looking at the proof and I saw that the transformation was defined as T(i) = Ti = (a c 0) and T(j) = Tj = (b d 0) [in this case i and j are the unit vectors]. However, the area of the parallelogram made between these vectors is stated to be as [[Ai x Aj]] (without the sinθ being θ the angle these vectors make). Or is it because as if they are unit vectors, they are 90 degrees to each other?

Thank you very much.

Edit: This link (around page 1) should help if I'm not clear with my explanations http://www.math.mun.ca/~mkondra/linalg2/la2set7.pdf
 
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You don't need the trig function to evaluate a cross product.
 
Oh darn, I finally saw my notes and checked that indeed it is just the vector product lv x wl (for the trig function, it involves the magnitude of both vectors or lal lbl sinθ, which is completely different from the vector product). So this means that we can as well find the area of that parallelogram using the sine of the angle and the two magnitudes?

Thank you Simon.
 
The advantage of the vector form is that it gives you the direction of the cross product as well.

Consider if ##\vec{v} = (v\cos\phi,v\sin\phi,0)^t## and ##\vec{u}=(u\cos\theta, u\sin\theta, 0)^t##
Where ##\theta## is the angle ##\vec{u}## makes to the x-axis and ##\phi## is the angle ##\vec v## makes to the x axis.

Then $$\vec{u}\times\vec{v} = \left| \begin{array}{ccc}
\hat{\imath} & \hat{\jmath} & \hat{k}\\
u\cos\theta & u\sin\theta & 0\\
v\cos\phi & v\cos\phi & 0\end{array}\right| = uv\sin(\phi-\theta)\hat{k}$$ ... which result required trig identities.

Notice that ## \theta -\phi ## is the angle between the vectors
- so the equation you are used to is just for the magnitude.

It gets trickier when you go to more than three dimensions.
 
Good morning I have been refreshing my memory about Leibniz differentiation of integrals and found some useful videos from digital-university.org on YouTube. Although the audio quality is poor and the speaker proceeds a bit slowly, the explanations and processes are clear. However, it seems that one video in the Leibniz rule series is missing. While the videos are still present on YouTube, the referring website no longer exists but is preserved on the internet archive...

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