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Space Vectors Problem 3.19 Determine the moment about the origin of the coordinate system, given a force vector and its distance from the origin. This requires vector multiplication! (Slides will advance automatically - or hit the space bar to advance slides.) 1 Problem 3.19 Determine the moment about the origin. • Given a force vector, F = 6i + 4j - 1k • This force vector acts on a point, A. • Given the distance from the origin to point A, this distance is represented as vector, r = -2i + 6j + 3k 2 y o x Begin with the coordinate system and the positive axes x, y, and z. z 3 y Draw the position vector for r that defines the distance from the origin, O, to point A. r = -2i + 6j + 3k -2 o x Beginning at the origin, on the x -axis, move 2 units to the left for the negative direction. z 4 y +6 r = -2i + 6j + 3k -2 x Now move 6 units up in the positive y -direction. z 5 y +3 +6 r = -2i + 6j + 3k -2 x Then move 3 units parallel to the z -axis in the positive direction. z 6 y A r r = -2i + 6j + 3k x O This locates point A. Represent this distance from the origin to point A as vector r. z 7 y Follow the same procedure to locate a force, F. A F = 6i + 4j - 1k r O z +6i x Along the x -axis, move 6 units to the right in the positive direction. 8 y A +4j r O z x +6i F = 6i + 4j - 1k Parallel to the y -axis, move 4 units up in the positive direction. 9 y A -1k +4j r O z x +6i F = 6i + 4j - 1k Parallel to the z -axis, move 1 unit toward the back, in the negative direction. 10 y A -1k F r O z +4j x +6i F = 6i + 4j - 1k This represents the position for the force vector, F. 11 y A F r O z x Note the orientation for the force vector, F, and its relative position with the distance vector, r. 12 y A F r O z x Keeping the same orientation, move the force vector, F, toward point A. 13 y A F r O z x Slide the force vector, F, until it passes through point A. 14 y F A r O z x Move the force, F, so that it acts through point A. Note the orientation of F and r. 15 y F r O z This force has components that are a perpendicular distance from the origin. This force then produces a moment about the fixed origin, which acts as the pivot or hinge point. x The moment about the origin is determined by vector multiplication, or the CROSS PRODUCT of these two vectors. 16 y F A To determine the moment, think about the starting point and moving toward the force. M =r x F r O x Distance from origin, O, to point A. r = OA = -2i + 6j + 3k z Force acting at point A, F = 6i + 4j - 1k 17 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k i j k -2 6 3 6 4 -1 18 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k (i) i j k -2 6 3 6 4 -1 6 3 4 -1 = 19 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k (i) i j k -2 6 3 6 4 -1 6 3 4 -1 = - (j) -2 3 6 -1 20 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k i j k -2 6 3 6 4 -1 6 (i) 4 = 3 -1 -2 - (j) 6 3 -1 + (k) -2 6 6 4 21 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k i j k -2 6 3 6 4 -1 6 (i) 4 = 3 -1 -2 - (j) 6 3 -1 + (k) -2 6 6 4 Now cross multiply the minor matrices. 22 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k i j k -2 6 3 6 4 -1 6 (i) 4 3 -1 For each minor matrix, take the product of these terms on this diagonal ... = -2 - (j) 6 3 -1 + (k) -2 6 6 4 (i) { (6x-1) - (3x4) } - (j) { (-2x-1) - (3x6) } + (k) { (-2x4) - (6x6) } 23 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k i j k -2 6 3 6 4 -1 6 (i) 4 3 -1 … then subtract the product of these terms on this diagonal. = -2 - (j) 6 3 -1 + (k) -2 6 6 4 (i) { (6x-1) - (3x4) } - (j) { (-2x-1) - (3x6) } + (k) { (-2x4) - (6x6) } 24 where M =r x F r = OA = -2i + 6j + 3k F = 6i + 4j - 1k i j k -2 6 3 6 4 -1 6 (i) 4 The final solution appears below. = 3 -2 -1 - (j) 6 3 -1 + (k) -2 6 6 4 (i) { (6x-1) - (3x4) } - (j) { (-2x-1) - (3x6) } + (k) { (-2x4) - (6x6) } M = - 18i + 16j - 44k 25