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Worked Examples · Example 6.5

Q.Find the torque of a force 7i^+3j^−5k^7\hat{i} + 3\hat{j} - 5\hat{k} about the origin. The force acts on a particle whose position vector is i^−j^+k^\hat{i} - \hat{j} + \hat{k}.

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Torque is calculated as the cross product of the position vector r⃗\vec{r} and the force vector F⃗\vec{F}, i.e., τ⃗=r⃗×F⃗\vec{\tau} = \vec{r} \times \vec{F}. For the given vectors, the torque is 2i^+12j^+10k^\boxed{2\hat{i} + 12\hat{j} + 10\hat{k}}.

When a force acts on an object, it can cause linear motion (translation) or rotational motion. Torque is the rotational equivalent of force; it's the physical quantity that causes an object to rotate about an axis.

The effectiveness of a force in causing rotation depends on three factors:

  1. Magnitude of the force: A larger force generally produces a larger torque.
  2. Distance from the pivot (axis of rotation): The further the force is applied from the pivot, the greater its rotational effect. This distance is represented by the position vector r⃗\vec{r} from the pivot to the point of application of the force.
  3. Angle between the force and the position vector: Only the component of the force perpendicular to the position vector contributes to rotation. If the force acts directly towards or away from the pivot, it causes no rotation.

The cross product (or vector product) is the mathematical operation that naturally combines these three factors. For two vectors A⃗\vec{A} and B⃗\vec{B}, their cross product A⃗×B⃗\vec{A} \times \vec{B} results in a new vector whose magnitude is ∣A⃗∣∣B⃗∣sin⁡θ|\vec{A}||\vec{B}|\sin\theta (where θ\theta is the angle between them) and whose direction is perpendicular to both A⃗\vec{A} and B⃗\vec{B} (given by the right-hand rule). This perfectly aligns with the definition of torque.

The torque τ⃗\vec{\tau} of a force F⃗\vec{F} acting at a position r⃗\vec{r} relative to the pivot point is given by:

τ⃗=r⃗×F⃗\vec{\tau} = \vec{r} \times \vec{F}

Let's apply this concept to the given problem.

  1. Identify the given vectors.

    The force vector is F⃗=7i^+3j^−5k^\vec{F} = 7\hat{i} + 3\hat{j} - 5\hat{k}.

    The position vector of the particle, relative to the origin (which is our pivot point for "about the origin"), is r⃗=i^−j^+k^\vec{r} = \hat{i} - \hat{j} + \hat{k}.

  2. Set up the cross product.

    We need to calculate τ⃗=r⃗×F⃗\vec{\tau} = \vec{r} \times \vec{F}. The cross product of two 3D vectors can be conveniently calculated using a determinant:

τ⃗=∣i^j^k^rxryrzFxFyFz∣\vec{\tau} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ r_x & r_y & r_z \\ F_x & F_y & F_z \end{vmatrix}

Substituting the components of $\vec{r}$ and $\vec{F}$:

τ⃗=∣i^j^k^1−1173−5∣\vec{\tau} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & 1 \\ 7 & 3 & -5 \end{vmatrix}

  1. Calculate the components of the torque vector. We expand the determinant along the first row:
    • i^\hat{i} component: …

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