Question Video: Using Vector Arithmetic and the Cross Product to Find the Moment of a Resultant Force about Two Points | Nagwa Question Video: Using Vector Arithmetic and the Cross Product to Find the Moment of a Resultant Force about Two Points | Nagwa

Question Video: Using Vector Arithmetic and the Cross Product to Find the Moment of a Resultant Force about Two Points Mathematics • Third Year of Secondary School

Given that 𝐅₁ = 2𝐢 − 𝐣, 𝐅₂ = 5𝐢 + 2𝐣, and 𝐅₃ = −3𝐢 + 2𝐣 are acting on the point 𝐴(1,1), determine the moment of the resultant of these forces about the two points 𝐵(2, 1) and 𝐶 (6, 4). Which of the following would we conclude about the line of action of the resultant force? [A] The line of action of the resultant force passes through both points 𝐵 and 𝐶. [B] The line of action of the resultant force is parallel to 𝐵𝐶. [C] The line of action of the resultant force passes through point 𝐵. [D] The line of action of the resultant force bisects 𝐵𝐶. [E] None of the answers are correct.

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Video Transcript

Given that 𝐅 one equals two 𝐢 minus 𝐣, 𝐅 two equals five 𝐢 plus two 𝐣, and 𝐅 three equals negative three 𝐢 plus two 𝐣 are acting on the point 𝐴 one, one, determine the moment of the resultant of these forces about the two points 𝐵 two, one and 𝐶 six, four. Which of the following would we conclude about the line of action of the resultant force?

The first step to solving this problem is to find the resultant of the forces acting on the point 𝐴. We can do this using simple vector addition of 𝐅 one, 𝐅 two, and 𝐅 three. The resultant force, which we will call 𝐅 𝑟, is equal to the sum 𝐅 one plus 𝐅 two plus 𝐅 three. So this comes to two 𝐢 minus 𝐣 plus five 𝐢 plus two 𝐣 minus three 𝐢 plus two 𝐣. Adding these component-wise gives us four 𝐢 plus three 𝐣. So we now have the resultant of the three forces 𝐅 𝑟 equals four 𝐢 plus three 𝐣.

We now need to find the moment of this resultant force about the two points 𝐵 and 𝐶, which we can find by taking the cross product 𝐫 cross 𝐅, where 𝐫 is the vector from the pivot point 𝑂 to the point of action 𝑃. For the moment about the point 𝐵, the vector 𝐫 is the vector 𝐵 to 𝐴, which is given by one, one minus two, one, which is equal to negative one, zero.

Therefore, the moment about the point 𝐵 is given by the determinant of the three-by-three matrix 𝑖, 𝑗, 𝑘, negative one, zero, zero, four, three, zero. Both 𝑟 and 𝐹 are in the 𝑥𝑦-plane with a 𝑘-component of zero. Therefore, only the 𝑘-component of their cross product will be nonzero.

Taking this determinant by expanding along the top row gives us negative three 𝑘. Let’s move this up here and clear a little space.

Now, for the moment about the point 𝐶, the vector 𝐫 is equal to the vector 𝐂𝚨, which is given by one, one minus six, four, which is equal to negative five, negative three. Therefore, the moment 𝑀 𝑐 of the resultant force about the point 𝐶 is given by the determinant of the three-by-three matrix 𝑖, 𝑗, 𝑘, negative five, negative three, zero, four, three, zero.

Once again, both vectors are in the 𝑥𝑦-plane and have a 𝑘-component of zero. Therefore, only the 𝑘-component of their cross product will be nonzero. Taking this determinant by expanding along the top row gives us once again negative three 𝑘.

We therefore have the first part of our answer. The moment of the resultant of the forces about the point 𝐵 is equal to negative three 𝑘 and about the point 𝐶 is also equal to negative three 𝑘.

Now, we need to decide which of the following options we can conclude about the line of action of the resultant force. To begin with, we know that all of the points involved are in the 𝑥𝑦-plane and all of the forces involved have no 𝑘-component. Therefore, we only need to consider the problem in two dimensions. We have two points 𝐵 and 𝐶, and the moment of the same force 𝐹 𝑟 equals four 𝑖 plus three 𝑗 is equal to negative three 𝑘 in both cases. It has the same magnitude and the same direction.

In both cases, the moment is directed into the screen. So, from this perspective, it is a clockwise-turning force. The line of action of the force must firstly be the same perpendicular distance from both points and must also be on the same side as both points, meaning that it does not pass between them.

We can therefore conclude answer (B) that the line of action of the resultant force is parallel to the line 𝐵𝐶.

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