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The distance between a carbon atom \(\left( {m = 12\;{\rm{u}}} \right)\) and an oxygen atom \(\left( {m = 16\;{\rm{u}}} \right)\) in the CO molecule is \({\bf{1}}{\bf{.13 \times 1}}{{\bf{0}}^{{\bf{10}}}}\;{\bf{m}}\) How far from the carbon atom is the center of mass of the molecule?

FIGURE 7-37Problem 50.

Short Answer

Expert verified

The center of mass of the mass system is at \(0.44\;{\rm{m}}\) from the \(1.00\;{\rm{kg}}\) mass.

Step by step solution

01

Given data

To find the center of mass, you have to find the relative positions of all particles for that particle, relative to which you measure the distance of the center of mass.

The given three masses are \({m_1} = 1.00\;{\rm{kg}}\), \({m_2} = 1.50\;{\rm{kg}}\), and \({m_3} = 1.10\;{\rm{kg}}\).

Now, the relative distance of \(1.50\;{\rm{kg}}\) from the \(1.00\;{\rm{kg}}\) mass is \({x_2} = 0.50\;{\rm{m}}\), and the relative distance of the \(1.10\;{\rm{kg}}\) from the \(1.00\;{\rm{kg}}\) mass is:

\(\begin{array}{c}{x_3} = \left( {0.50\;{\rm{m}} + 0.25\;{\rm{m}}} \right)\\ = 0.75\;{\rm{m}}\end{array}\)

02

Calculation of the center of mass

Now, the center of mass of the mass system is:

\(\begin{array}{c}{x_{{\rm{CM}}}} = \frac{{\left( {{m_1} \times {x_1}} \right) + \left( {{m_2} \times {x_2}} \right) + \left( {{m_2} \times {x_2}} \right)}}{{{m_1} + {m_2} + {m_3}}}\\ = \frac{{\left( {1.00\;{\rm{kg}} \times 0} \right) + \left( {1.50\;{\rm{kg}} \times 0.50\;{\rm{m}}} \right) + \left( {1.10\;{\rm{kg}} \times 0.75\;{\rm{m}}} \right)}}{{1.00\;{\rm{kg}} + 1.50\;{\rm{kg}} + 1.10\;{\rm{kg}}}}\\ = 0.44\;{\rm{m}}\end{array}\)

Hence, the center of mass of the mass system is at \(0.44\;{\rm{m}}\) from the \(1.00\;{\rm{kg}}\) mass.

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Most popular questions from this chapter

(I) A constant friction force of 25 N acts on a 65-kg skier for 15 s on level snow. What is the skier’s change in velocity?

(a) Calculate the impulse experienced when a 55-kg person lands on firm ground after jumping from a height of 2.8 m.

(b) Estimate the average force exerted on the person’s feet by the ground if the landing is stiff-legged, and again

(c) with bent legs. With stiff legs, assume the body moves 1.0 cm during impact, and when the legs are bent, about 50 cm. [Hint: The average net force on him, which is related to impulse, is the vector sum of gravity and the force exerted by the ground. See Fig. 7–34.] We will see in Chapter 9 that the force in (b) exceeds the ultimate strength of bone (Table 9–2).

FIGURE 7-34 Problem 24.

A 28-g rifle bullet travelling\(190\;{\rm{m/s}}\)embeds itself in a 3.1-kg pendulum hanging on a 2.8-m-long string, which makes the pendulum swing upward in an arc. Determine the vertical and horizontal components of the pendulum’s maximum displacement.

A 0.060-kg tennis ball, moving with a speed of 5.50 m/s has a head-on collision with a 0.090-kg ball initially moving in the same direction at a speed of 3.00 m/s. Assuming a perfectly elastic collision, determine the speed and direction of each ball after the collision?

A pendulum consists of a mass M hanging at the bottom end of a massless rod of length l which has a frictionless pivot at its top end. A mass m, moving as shown in Fig. 7–35 with velocity v, impacts M and becomes embedded. What is the smallest value of v sufficient to cause the pendulum (with embedded mass m) to swing clear over the top of its arc?

FIGURE 7-35Problem 42.

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