27 Further Applications of Newton’s Laws of Motion

Suppose two tugboats push on a barge at different angles, as shown in (Figure). The first tugboat exerts a force of \(2.7×{\text{10}}^{5}\phantom{\rule{0.25em}{0ex}}\text{N}\) in the x-direction, and the second tugboat exerts a force of \(3.6×{\text{10}}^{5}\phantom{\rule{0.25em}{0ex}}\text{N}\) in the y-direction.

If the mass of the barge is \(5.0×{\text{10}}^{6}\phantom{\rule{0.25em}{0ex}}\text{kg}\) and its acceleration is observed to be \(7\text{.}\text{5}×{\text{10}}^{-2}\phantom{\rule{0.25em}{0ex}}{\text{m/s}}^{2}\) in the direction shown, what is the drag force of the water on the barge resisting the motion? (Note: drag force is a frictional force exerted by fluids, such as air or water. The drag force opposes the motion of the object.)

Strategy

The directions and magnitudes of acceleration and the applied forces are given in (Figure)(a). We will define the total force of the tugboats on the barge as \({\mathbf{\text{F}}}_{\text{app}}\) so that:

Since the barge is flat bottomed, the drag of the water \({\mathbf{\text{F}}}_{\text{D}}\) will be in the direction opposite to \({\mathbf{\text{F}}}_{\text{app}}\), as shown in the free-body diagram in (Figure)(b). The system of interest here is the barge, since the forces on it are given as well as its acceleration. Our strategy is to find the magnitude and direction of the net applied force \({\mathbf{\text{F}}}_{\text{app}}\), and then apply Newton’s second law to solve for the drag force \({\mathbf{\text{F}}}_{\text{D}}\).

Solution

Since \({\mathbf{\text{F}}}_{x}\) and \({\mathbf{\text{F}}}_{y}\) are perpendicular, the magnitude and direction of \({\mathbf{\text{F}}}_{\text{app}}\) are easily found. First, the resultant magnitude is given by the Pythagorean theorem:

The angle is given by

which we know, because of Newton’s first law, is the same direction as the acceleration. \({\mathbf{\text{F}}}_{\text{D}}\) is in the opposite direction of \({\mathbf{\text{F}}}_{\text{app}}\), since it acts to slow down the acceleration. Therefore, the net external force is in the same direction as \({\mathbf{\text{F}}}_{\text{app}}\), but its magnitude is slightly less than \({\mathbf{\text{F}}}_{\text{app}}\). The problem is now one-dimensional. From (Figure)(b), we can see that

But Newton’s second law states that

Thus,

This can be solved for the magnitude of the drag force of the water \({F}_{\text{D}}\) in terms of known quantities:

Substituting known values gives

The direction of \({\mathbf{\text{F}}}_{\text{D}}\) has already been determined to be in the direction opposite to \({\mathbf{\text{F}}}_{\text{app}}\), or at an angle of \(\text{53º}\) south of west.

Discussion

The numbers used in this example are reasonable for a moderately large barge. It is certainly difficult to obtain larger accelerations with tugboats, and small speeds are desirable to avoid running the barge into the docks. Drag is relatively small for a well-designed hull at low speeds, consistent with the answer to this example, where \({F}_{\text{D}}\) is less than 1/600th of the weight of the ship.

Consider the traffic light (mass 15.0 kg) suspended from two wires as shown in (Figure). Find the tension in each wire, neglecting the masses of the wires.

Strategy

The system of interest is the traffic light, and its free-body diagram is shown in (Figure)(c). The three forces involved are not parallel, and so they must be projected onto a coordinate system. The most convenient coordinate system has one axis vertical and one horizontal, and the vector projections on it are shown in part (d) of the figure. There are two unknowns in this problem (\({T}_{1}\) and \({T}_{2}\)), so two equations are needed to find them. These two equations come from applying Newton’s second law along the vertical and horizontal axes, noting that the net external force is zero along each axis because acceleration is zero.

Solution

First consider the horizontal or x-axis:

Thus, as you might expect,

This gives us the following relationship between \({T}_{1}\) and \({T}_{2}\):

Thus,

Note that \({T}_{1}\) and \({T}_{2}\) are not equal in this case, because the angles on either side are not equal. It is reasonable that \({T}_{2}\) ends up being greater than \({T}_{1}\), because it is exerted more vertically than \({T}_{1}\).

Now consider the force components along the vertical or y-axis:

This implies

Substituting the expressions for the vertical components gives

There are two unknowns in this equation, but substituting the expression for \({T}_{2}\) in terms of \({T}_{1}\) reduces this to one equation with one unknown:

which yields

Solving this last equation gives the magnitude of \({T}_{1}\) to be

Finally, the magnitude of \({T}_{2}\) is determined using the relationship between them, \({T}_{2}\) = 1.225 \({T}_{1}\), found above. Thus we obtain

Discussion

Both tensions would be larger if both wires were more horizontal, and they will be equal if and only if the angles on either side are the same (as they were in the earlier example of a tightrope walker).

(Figure) shows a 75.0-kg man (weight of about 165 lb) standing on a bathroom scale in an elevator. Calculate the scale reading: (a) if the elevator accelerates upward at a rate of \(1\text{.}{\text{20 m/s}}^{2}\), and (b) if the elevator moves upward at a constant speed of 1 m/s.

Strategy

If the scale is accurate, its reading will equal \({F}_{\text{p}}\), the magnitude of the force the person exerts downward on it. (Figure)(a) shows the numerous forces acting on the elevator, scale, and person. It makes this one-dimensional problem look much more formidable than if the person is chosen to be the system of interest and a free-body diagram is drawn as in (Figure)(b). Analysis of the free-body diagram using Newton’s laws can produce answers to both parts (a) and (b) of this example, as well as some other questions that might arise. The only forces acting on the person are his weight \(\mathbf{\text{w}}\) and the upward force of the scale \({\mathbf{\text{F}}}_{\text{s}}\). According to Newton’s third law \({\mathbf{\text{F}}}_{\text{p}}\) and \({\mathbf{\text{F}}}_{\text{s}}\) are equal in magnitude and opposite in direction, so that we need to find \({F}_{\text{s}}\) in order to find what the scale reads. We can do this, as usual, by applying Newton’s second law,

From the free-body diagram we see that \({F}_{\text{net}}={F}_{\text{s}}-w\), so that

Solving for \({F}_{\text{s}}\) gives an equation with only one unknown:

or, because \(w=\mathrm{mg}\), simply

No assumptions were made about the acceleration, and so this solution should be valid for a variety of accelerations in addition to the ones in this exercise.

Solution for (a)

In this part of the problem, \(a=1.20\phantom{\rule{0.25em}{0ex}}{\text{m/s}}^{2}\), so that

yielding

Discussion for (a)

This is about 185 lb. What would the scale have read if he were stationary? Since his acceleration would be zero, the force of the scale would be equal to his weight:

So, the scale reading in the elevator is greater than his 735-N (165 lb) weight. This means that the scale is pushing up on the person with a force greater than his weight, as it must in order to accelerate him upward. Clearly, the greater the acceleration of the elevator, the greater the scale reading, consistent with what you feel in rapidly accelerating versus slowly accelerating elevators.

Solution for (b)

Now, what happens when the elevator reaches a constant upward velocity? Will the scale still read more than his weight? For any constant velocity—up, down, or stationary—acceleration is zero because \(a=\frac{\Delta v}{\Delta t}\), and \(\Delta v=0\).

Thus,

Now

which gives

Discussion for (b)

The scale reading is 735 N, which equals the person’s weight. This will be the case whenever the elevator has a constant velocity—moving up, moving down, or stationary.