hholzer
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I am reading through David Widder's Advanced Calculus and he abbreviates a determinant
as:
<br /> <br /> \left( \begin{array}{cccc} <br /> <br /> r_{1} \ s_{1} \ t_{1}\\ <br /> <br /> r_{2} \ s_{2} \ t_{2}\\ <br /> <br /> r_{3} \ s_{3} \ t_{3}\\ <br /> <br /> \end{array} \right)<br />
And refers to it by (rst). He then states that expanding by the minors of a given
column, we have:
<br /> <br /> (rst) = r \cdot (s \times t) = s \cdot (t \times r) = t \cdot (r \times s) <br /> <br />
Now, I worked it out by looking at the cofactors of r_1, r_2, and r_3 which are the components of the vector (s x t) and confirmed it holds. But how can I see
this property without having to do that? Is there another way to see this say algebraically or geometrically? Some more intuitive way, perhaps?
as:
<br /> <br /> \left( \begin{array}{cccc} <br /> <br /> r_{1} \ s_{1} \ t_{1}\\ <br /> <br /> r_{2} \ s_{2} \ t_{2}\\ <br /> <br /> r_{3} \ s_{3} \ t_{3}\\ <br /> <br /> \end{array} \right)<br />
And refers to it by (rst). He then states that expanding by the minors of a given
column, we have:
<br /> <br /> (rst) = r \cdot (s \times t) = s \cdot (t \times r) = t \cdot (r \times s) <br /> <br />
Now, I worked it out by looking at the cofactors of r_1, r_2, and r_3 which are the components of the vector (s x t) and confirmed it holds. But how can I see
this property without having to do that? Is there another way to see this say algebraically or geometrically? Some more intuitive way, perhaps?