Question 3.SP.9: Four tugboats are bringing an ocean liner to its pier. Each ......

Four tugboats are bringing an ocean liner to its pier. Each tugboat exerts a 5000-lb force in the direction shown. Determine (a) the equivalent forcecouple system at the foremast O, (b) the point on the hull where a single, more powerful tugboat should push to produce the same effect as the original four tugboats.

STRATEGY: The equivalent force-couple system is defined by the sum of the given forces and the sum of the moments of those forces at a particular point. A single tugboat could produce this system by exerting the resultant force at a point of application that produces an equivalent moment.

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In this problem, we are given a system of forces and we need to find the equivalent force-couple system at point O.
Step 1:
Resolve each of the given forces into components. We can break down each force vector into its x and y components using the given values.
Step 2:
Find the resultant force R. To find the resultant force, we add up all the individual force components.
Step 3:
Find the moment of each force component about point O. We can calculate the moment of each force component by taking the cross product of the position vector and the force vector.
Step 4:
Find the equivalent couple moment at point O. To find the equivalent couple moment, we add up all the individual moments of the force components.
Step 5:
Write the equivalent force-couple system at point O. The equivalent force-couple system consists of a force R and a couple moment M_O^R.
Step 6:
Interpret the results. We can interpret the results by expressing the force and couple moment in different forms, such as in vector form or in magnitude-angle form.
Step 7:
In part b of the problem, we are asked to consider a single tugboat that exerts a force equal to R at point A. We need to find the position of point A such that the moment of R about point O is equal to M_O^R.
Step 8:
Define the position vector r of point A. We can define the position vector r as a combination of the x and y components of point A.
Step 9:
Use the cross product to find the moment of R about point O. We can take the cross product of the position vector r and the force vector R to find the moment of R about point O.
Step 10:
Set up an equation and solve for the position of point A. By equating the moment of R about point O to M_O^R, we can solve for the position of point A.
Step 11:
Finally, we reflect on the problem and think about how reducing the given situation to a single force (R) and a single point of application (A) makes it easier to understand the overall effect of the tugboats in maneuvering the ocean liner. However, in practical terms, having four boats applying force allows for greater control in slowing and turning a large ship in a crowded harbor.

Final Answer

MODELING and ANALYSIS:

a. Force-Couple System at O. Resolve each of the given forces into components, as in Fig. 1 (kip units are used). The force-couple system at O equivalent to the given system of forces consists of a force R and a couple \mathbf{M}_O^R defined as

\begin{aligned}\mathbf{R} & =\Sigma \mathbf{F} \\& =(2.50 \mathbf{i}-4.33 \mathbf{j})+(3.00 \mathbf{i}-4.00 \mathbf{j})+(-5.00 \mathbf{j})+(3.54 \mathbf{i}+3.54 \mathbf{j}) \\& =9.04 \mathbf{i}-9.79 \mathbf{j}\end{aligned}

\begin{aligned}\mathbf{M}_O^R= & \Sigma(\mathbf{r} \times \mathbf{F}) \\= & (-90 \mathbf{i}+50 \mathbf{j}) \times(2.50 \mathbf{i}-4.33 \mathbf{j}) \\& +(100 \mathbf{i}+70 \mathbf{j}) \times(3.00 \mathbf{i}-4.00 \mathbf{j}) \\& +(400 \mathbf{i}+70 \mathbf{j}) \times(-5.00 \mathbf{j}) \\& +(300 \mathbf{i}-70 \mathbf{j}) \times(3.54 \mathbf{i}+3.54 \mathbf{j}) \\= & (390-125-400-210-2000+1062+248) \mathbf{k} \\= & -1035 \mathbf{k}\end{aligned}

The equivalent force-couple system at O is thus (Fig. 2)

\mathbf{R}=(9.04 ~\mathrm{kips}) \mathbf{i}-(9.79 ~\mathrm{kips}) \mathbf{j} \quad \mathbf{M}_O^R=-(1035 ~\mathrm{kip} \cdot \mathrm{ft}) \mathbf{k}

or

\mathbf{R}=13.33 ~\mathrm{kips} \angle47.3^{\circ} \quad \mathbf{M}_O^R=1035 ~\mathrm{kip} \cdot \mathrm{ft}

Remark: Since all the forces are contained in the plane of the figure, you would expect the sum of their moments to be perpendicular to that plane. Note that you could obtain the moment of each force component directly from the diagram by first forming the product of its magnitude and perpendicular distance to O and then assigning to this product a positive or a negative sign, depending upon the sense of the moment.

b. Single Tugboat. The force exerted by a single tugboat must be equal to R, and its point of application A must be such that the moment of R about O is equal to \mathbf{M}_O^R (Fig. 3). Observing that the position vector of A is

\mathbf{r}=x \mathbf{i}+70 \mathbf{j}

you have

\begin{aligned}\mathbf{r} \times \mathbf{R} & =\mathbf{M}_O^R \\(x \mathbf{i}+70 \mathbf{j}) \times(9.04 \mathbf{i}-9.79 \mathbf{j}) & =-1035 \mathbf{k} \\-x(9.79) \mathbf{k}-633 \mathbf{k} & =-1035 \mathbf{k} \quad x=41.1 ~\mathrm{ft}\end{aligned}

REFLECT and THINK: Reducing the given situation to that of a single force makes it easier to visualize the overall effect of the tugboats in maneuvering the ocean liner. But in practical terms, having four boats applying force allows for greater control in slowing and turning a large ship in a crowded harbor.

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