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A force \(\vec{F} = 2\hat{i} - \lambda\hat{j} + 5\hat{k}\) is applied at the point A\((1, 2, 5)\). If its moment about the point B\((-1,-2, 3)\) is \(16\hat{i} - 6\hat{j}+2\lambda\hat{k}\), then what is the value of \(\lambda\)?

This question was previously asked in
NDA 2 2025 GAT Question Paper (14-Sep-2025)
The correct answer is
-2

Understanding the Moment of a Force

The problem asks us to find the value of '\(\lambda\)' given a force vector '\(\vec{F}\)', a point of application A, a point B about which the moment is calculated, and the resulting moment vector '\(\vec{M}\)'.

The moment of a force '\(\vec{F}\)' about a point B, when the force is applied at point A, is defined as the cross product of the position vector '\(\vec{r}\)' (from B to A) and the force vector '\(\vec{F}\)'. Mathematically, this is expressed as:

\(\vec{M} = \vec{r} \times \vec{F}\)

where '\(\vec{r} = \vec{A} - \vec{B}\)'.

Calculating the Position Vector

First, we need to determine the position vector '\(\vec{r}\)' from point B\((-1, -2, 3)\) to point A\((1, 2, 5)\).

The coordinates of A are \((x_A, y_A, z_A) = (1, 2, 5)\).

The coordinates of B are \((x_B, y_B, z_B) = (-1, -2, 3)\).

The position vector '\(\vec{r}\)' is calculated as:

\(\vec{r} = (x_A - x_B)\hat{i} + (y_A - y_B)\hat{j} + (z_A - z_B)\hat{k}\) \(\vec{r} = (1 - (-1))\hat{i} + (2 - (-2))\hat{j} + (5 - 3)\hat{k}\) \(\vec{r} = (1 + 1)\hat{i} + (2 + 2)\hat{j} + (2)\hat{k}\) \(\vec{r} = 2\hat{i} + 4\hat{j} + 2\hat{k}\)

Calculating the Moment Vector

Now, we calculate the moment vector '\(\vec{M}\)' using the cross product '\(\vec{r} \times \vec{F}\)'.

We have:

\(\vec{r} = 2\hat{i} + 4\hat{j} + 2\hat{k}\) \(\vec{F} = 2\hat{i} - \lambda\hat{j} + 5\hat{k}\)

The cross product can be computed using a determinant:

$ \vec{M} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 4 & 2 \\ 2 & -\lambda & 5 \end{vmatrix} $

Expanding the determinant:

\(\vec{M} = \hat{i}((4)(5) - (2)(-\lambda)) - \hat{j}((2)(5) - (2)(2)) + \hat{k}((2)(-\lambda) - (4)(2))\) \(\vec{M} = \hat{i}(20 + 2\lambda) - \hat{j}(10 - 4) + \hat{k}(-2\lambda - 8)\) \(\vec{M} = (20 + 2\lambda)\hat{i} - 6\hat{j} + (-2\lambda - 8)\hat{k}\)

Finding the Value of Lambda (\(\lambda\))

We are given that the moment vector is '\(\vec{M}_{given} = 16\hat{i} - 6\hat{j} + 2\lambda\hat{k}\)'.

By comparing the calculated moment vector '\(\vec{M}\)' with the given moment vector '\(\vec{M}_{given}\)', we equate their corresponding components:

  • X-component: '\((20 + 2\lambda) = 16\)'
  • Y-component: '\(-6 = -6\)' (This confirms our calculation for the j-component)
  • Z-component: '\((-2\lambda - 8) = 2\lambda\)'

Let's solve the equation from the X-component:

\(20 + 2\lambda = 16\) \(2\lambda = 16 - 20\) \(2\lambda = -4\) \(\lambda = \frac{-4}{2}\) \(\lambda = -2\)

We can verify this using the Z-component equation:

\(-2\lambda - 8 = 2\lambda\) \(-8 = 2\lambda + 2\lambda\) \(-8 = 4\lambda\) \(\lambda = \frac{-8}{4}\) \(\lambda = -2\)

Both component equations yield the same value for '\(\lambda\)'.

Conclusion

The value of '\(\lambda\)' that satisfies the condition for the moment of the force is -2.

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