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NCERT Exemplar · Q19

Q.The vector sum of a system of non-collinear forces acting on a rigid body is given to be non-zero. If the vector sum of all the torques due to the system of forces about a certain point is found to be zero, does this mean that it is necessarily zero about any arbitrary point?

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When non-collinear forces on a rigid body have a non-zero resultant but zero torque about one point, the torque about any other point is generally non-zero. The torque depends on the choice of origin when the net force is non-zero.

The heart of this question lies in understanding how torque transforms when you change your reference point. Torque is not an intrinsic property of a force system alone—it depends on where you measure it from. When the net force is zero, torque becomes independent of the reference point (a pure couple). But when the net force is non-zero, shifting your reference point changes the torque.

Let's see why this happens mathematically and physically.

Why torque depends on the reference point

Torque measures the turning effect of forces about a chosen point. For a force F⃗i\vec{F}_i acting at position r⃗i\vec{r}_i (measured from point OO), the torque is:

τ⃗i=r⃗i×F⃗i\vec{\tau}_i = \vec{r}_i \times \vec{F}_i

The total torque about OO is:

τ⃗O=∑ir⃗i×F⃗i\vec{\tau}_O = \sum_i \vec{r}_i \times \vec{F}_i

Now suppose we measure torques about a different point O′O', displaced from OO by vector a⃗\vec{a}. The position of the same force application point relative to O′O' is r⃗i′=r⃗i−a⃗\vec{r}_i' = \vec{r}_i - \vec{a}.

The torque about O′O' becomes:

τ⃗O′=∑ir⃗i′×F⃗i=∑i(r⃗i−a⃗)×F⃗i\vec{\tau}_{O'} = \sum_i \vec{r}_i' \times \vec{F}_i = \sum_i (\vec{r}_i - \vec{a}) \times \vec{F}_i

Expanding:

τ⃗O′=∑ir⃗i×F⃗i−∑ia⃗×F⃗i\vec{\tau}_{O'} = \sum_i \vec{r}_i \times \vec{F}_i - \sum_i \vec{a} \times \vec{F}_i

τ⃗O′=τ⃗O−a⃗×∑iF⃗i\vec{\tau}_{O'} = \vec{\tau}_O - \vec{a} \times \sum_i \vec{F}_i

τ⃗O′=τ⃗O−a⃗×F⃗net\vec{\tau}_{O'} = \vec{\tau}_O - \vec{a} \times \vec{F}_{\text{net}}

This is the key relationship. The torque about a new point equals the old torque minus the cross product of the displacement with the net force.

Applying to our problem

  1. Given conditions: We have F⃗net=∑iF⃗i≠0⃗\vec{F}_{\text{net}} = \sum_i \vec{F}_i \neq \vec{0} and τ⃗O=0⃗\vec{\tau}_O = \vec{0} about some particular point OO.

  2. Torque about an arbitrary point O′O': Using the transformation formula:

τ⃗O′=0⃗−a⃗×F⃗net=−a⃗×F⃗net\vec{\tau}_{O'} = \vec{0} - \vec{a} \times \vec{F}_{\text{net}} = -\vec{a} \times \vec{F}_{\text{net}}

  1. Is this zero? The cross product a⃗×F⃗net\vec{a} \times \vec{F}_{\text{net}} is zero only if:
    • a⃗=0⃗\vec{a} = \vec{0} (we haven't moved; O′=OO' = O), or
    • a⃗\vec{a} is parallel to F⃗net\vec{F}_{\text{net}} …

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