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Systems of Particles and Rotational Motion

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Question : 5 of 33
Marks: +1, -0
Show that a→.(b→×c→)\overset{\rightarrow}{a}.\left(\overset{\rightarrow}{b}\times\overset{\rightarrow}{c}\right) is equal in magnitude to the volume of the parallelepiped formed on the three vectors, a→,b→\overset{\rightarrow}{a},\overset{\rightarrow}{b} and c→\overset{\rightarrow}{c}
Solution:  
Let a parallelopiped be formed on the three vectors
OA→=a→,OB→=b→\overset{\rightarrow}{OA}=\overset{\rightarrow}{a}, \overset{\rightarrow}{OB}=\overset{\rightarrow}{b}and OC→=c→\overset{\rightarrow}{OC}=\overset{\rightarrow}{c}
Now, b→×c→=bcsin⁡90∘n^=bcn^\overset{\rightarrow}{b}\times\overset{\rightarrow}{c}=bc\sin 90^{\circ}\hat{n}=bc\hat{n}
where n^\hat{n} is unit vector along OA→\overset{\rightarrow}{OA} perpendicular to the plane containing b→\overset{\rightarrow}{b} and c→.\overset{\rightarrow}{c}.
Now a→.(b→×c→)\overset{\rightarrow}{a}.\left(\overset{\rightarrow}{b}\times\overset{\rightarrow}{c}\right) =a→.bcn^=(a)(bc)cos⁡0∘=abc=\overset{\rightarrow}{a}. bc\hat{n}=(a)(bc)\cos 0^{\circ}=abc
which is equal in magnitude to the volume of the parallelopiped.
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