Moment of a force (i.e., Torque) about a point

Vector of Class 11

Consider a force acting at point A whose position vector is , then moment of force (i.e, torque) about point O is given by

= (yFz − zFy) + (zFx − xFz) + (xFy − yFx)

Physically represents the tendency of the force to rotate the body (on which it acts) about an axis which passes through O and perpendicular to the plane containing the force and position vector .

Moment of  a force (i.e., Torque) about a point

Moment of Force About a Line

Consider a force

acting at a point a whose position vector is

. Then moment of about point O is given by

Then the component of in the direction of vector (i.e., ) is called the moment of force about a line and is given by

= Moment of  a force (i.e., Torque) about a point

where is unit vector along . In particular if line OL coincides with the x-axis, then

but this is the component of along x-axis

Illustration 18.A force vector Moment of  a force (i.e., Torque) about a point passes through a point (2, 5, 7). Prove that force passes through the origin.

Solution:If the force passes through the origin, its moment about the origin will be zero.

Moment of force (Torque) =

Illustration 19.Determine the torque of the 20 N force (in XY-plane) about point O as shown in figure.

Solution:

= () (20) (5 cos 30°)

= −86.6 Nm

Illustration 20.Find the perpendicular distance from the point (1, 2, 3) to the line joining from the origin to the point (2, 10, 5).

Solution:

Moment of  a force (i.e., Torque) about a point

perpendicular distance = AB

Moment of  a force (i.e., Torque) about a point

∴AB = 1.84 units

Illustration 21.Determine the resultant of the four forces tangent to the circle of radius 3 m as shown in the figure. What will be its location with respect to the centre of the circle.

Moment of  a force (i.e., Torque) about a point

Solution:Resolve forces along x and y axis

ΣFx = 150 − 100 cos 45° = 150 − 70.7 = + 79.3 N

ΣFy = 50 − 80 − 100 cos 45° = 50 − 80 − 70.7 = −100.7 N

∴ Resultant force = Moment of  a force (i.e., Torque) about a point

F = 128 N

The torque of Moment of  a force (i.e., Torque) about a point about O is and it equals the sum of the torque of all the given forces about O. Hence

128r = 50(3) – 150(3) + 80(3) − 100(3)

= −360

∴r = 2.81 m

Hence the resultant force of 128 N acts at a distance of 2.81 m form O causing −ve torque.

Illustration 22.A cube of side a is acted upon by a force as shown. Find the moment of (a) about point A (b) about the diagonal AG of the cube.

Solution:(a) Moment of  a force (i.e., Torque) about a point

Moment of about point A is

Moment of  a force (i.e., Torque) about a point

(b) Moment of  a force (i.e., Torque) about a point

unit vector along Moment of  a force (i.e., Torque) about a point =

Moment of about line AG is

Moment of  a force (i.e., Torque) about a point

Illustration 23.Two vectors in which one has magnitude twice that of the other, act on a particle. Find the angle between them, if their resultant is perpendicular to the first vector.

Solution:Let the vector Moment of  a force (i.e., Torque) about a point has magnitude twice that of Moment of  a force (i.e., Torque) about a point ; |Moment of  a force (i.e., Torque) about a point | = 2|Moment of  a force (i.e., Torque) about a point |

SinceMoment of  a force (i.e., Torque) about a point , φ = 900,

substituting φ = 900 in φ = tan-1Moment of  a force (i.e., Torque) about a point

we have |Moment of  a force (i.e., Torque) about a point | + |Moment of  a force (i.e., Torque) about a point | cos θ = 0. This gives

θ = cos-1Moment of  a force (i.e., Torque) about a point ; substituting |Moment of  a force (i.e., Torque) about a point | =

we have θ = 1200.

Moment of  a force (i.e., Torque) about a point

Illustration 24.If five consecutive sides of a regular hexagon represent five unit vectors acting in the same sense, find their resultant vector.

Solution:It is relevant from the vector diagram that each vector derivates from its neighbour by an angle of 600. We bring the tails of each vector to a point (origin) and observe that and Moment of  a force (i.e., Torque) about a point are equal and opposite; and Moment of  a force (i.e., Torque) about a point and Moment of  a force (i.e., Torque) about a point are equal and opposite.

Moment of  a force (i.e., Torque) about a point

Moment of  a force (i.e., Torque) about a point

Illustration 25.An insect moves in a circular path of radius R. if it rotates through an angle θ, find its displacement.

Solution:When the insect moves from position 1 to position 2, the displacement s = change in position vector Moment of  a force (i.e., Torque) about a point Since Moment of  a force (i.e., Torque) about a point . the magnitude of the displacement is

|Moment of  a force (i.e., Torque) about a point

since the insect moves in a circular path,

r1 = r2 = R

Hence |Moment of  a force (i.e., Torque) about a point | = 2R sin θ/2. The direction of Moment of  a force (i.e., Torque) about a point is given as β = π/2 + θ/2, as shown in the figure.

Moment of  a force (i.e., Torque) about a point

Illustration 26.Find the vector equation of a line which is parallel to a given vector Moment of  a force (i.e., Torque) about a point and passes through a given point P having position vectorMoment of  a force (i.e., Torque) about a point .

Solution:Let us draw a straight line PQ which is given by Moment of  a force (i.e., Torque) about a point

 

 

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