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Exercises · 5.11

Q.A body constrained to move along the zz-axis of a coordinate system is subject to a constant force F⃗\vec{F} given by
[!FORMULA] F⃗=−i^+2j^+3k^ N\vec{F} = -\hat{i} + 2\hat{j} + 3\hat{k}\ \text{N}
where i^,j^,k^\hat{i}, \hat{j}, \hat{k} are unit vectors along the xx-, yy- and zz-axis of the system respectively. What is the work done by this force in moving the body a distance of 4 m4\ \text{m} along the zz-axis?

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The work done by a force is the product of the force component parallel to the displacement and the magnitude of the displacement. For a displacement purely along the zz-axis, only the zz-component of the force does work, resulting in a work done of 12 J\boxed{12\ \text{J}}.

In physics, work is a measure of energy transfer that occurs when a force acts on an object, causing it to move through a distance. Crucially, not all parts of a force contribute to the work done. Only the component of the force that acts in the direction of the displacement (or opposite to it) actually does work. Any component of the force perpendicular to the displacement does no work.

Imagine pushing a box across a floor. If you push it horizontally, you do work. If you also push downwards on the box, that downward force component does no work because the box is not moving downwards; it's moving horizontally.

Mathematically, this concept is elegantly captured by the dot product (also known as the scalar product) of the force vector and the displacement vector. The dot product inherently selects the component of one vector that is parallel to the other.

The work done WW by a constant force F⃗\vec{F} causing a displacement d⃗\vec{d} is given by:

W=F⃗⋅d⃗W = \vec{F} \cdot \vec{d}

In component form, if F⃗=Fxi^+Fyj^+Fzk^\vec{F} = F_x\hat{i} + F_y\hat{j} + F_z\hat{k} and d⃗=dxi^+dyj^+dzk^\vec{d} = d_x\hat{i} + d_y\hat{j} + d_z\hat{k}, then:

W=Fxdx+Fydy+FzdzW = F_x d_x + F_y d_y + F_z d_z

Let's apply this to the given problem.

  1. Identify the Force Vector (F⃗\vec{F}): The problem states the constant force acting on the body is:

F⃗=−i^+2j^+3k^ N\vec{F} = -\hat{i} + 2\hat{j} + 3\hat{k}\ \text{N}

This means the force has a component of $-1\ \text{N}$ along the $x$-axis, $2\ \text{N}$ along the $y$-axis, and $3\ \text{N}$ along the $z$-axis.

2. Determine the Displacement Vector (d⃗\vec{d}):

The body is constrained to move along the zz-axis and moves a distance of 4 m4\ \text{m} along it. This means the displacement is entirely in the positive zz-direction.

Therefore, the displacement vector is:

d⃗=0i^+0j^+4k^=4k^ m\vec{d} = 0\hat{i} + 0\hat{j} + 4\hat{k} = 4\hat{k}\ \text{m}

  1. Calculate the Work Done using the Dot Product: Now we use the formula for work done, W=F⃗⋅d⃗W = \vec{F} \cdot \vec{d}. Substitute the identified force and displacement vectors:

W=(−i^+2j^+3k^)⋅(4k^)W = (-\hat{i} + 2\hat{j} + 3\hat{k}) \cdot (4\hat{k})

To compute the dot product, we multiply the corresponding components and sum them up. Recall that for orthogonal unit vectors: …

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