06 Resultant of Force Problem Set

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RESULTANT OF A FORCE | PRACTICE PROBLEMS Complete the following to reinforce your understanding of the concept covered in this module.

PROBLEM 1: A force system is shown below. What is the resultant magnitude and resultant direction of the three forces?

A. 19.83 𝑙𝑏; 14.09° B. 19.83 𝑙𝑏; 24.09° C. 29.83 𝑙𝑏; 14.09° D. 29.83 𝑙𝑏; 24.09°



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SOLUTION 1: The topic of the RESULTANT OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing.

This problem requires us to break each individual force up into components, sum them together, and then plug those components in the formula to calculate the resultant. The first step in this problem is to define our Coordinate System. When working with two-dimensional problems, it is typical to use a Cartesian Coordinate System such that the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 represents the horizontal component, and the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 represents the vertical component.



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The next step is to cycle through each individual force, one at a time, and break the force into its horizontal and vertical components. We will start with the 100 𝑁 force highlighted in red.

The line of action of the force is provided, as well as the direction of the angle relative to the origin, given as 30°. We can then use this angle to determine the components.



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We will use trigonometric identities to solve for each of the components. We can identify the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 as our adjacent side, đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 as our opposite side, and the force vector as our hypotenuse.

Calculating the horizontal component, we use the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 to represent the horizontal component of the force. Solving for the horizontal component of the force, we find: 𝐹6788 = (100 𝑙𝑏)(cos 30°) = 86.6 𝑙𝑏



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Moving on to the vertical component, we use the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 to represent the vertical component of the force.

Solving for the vertical component of the force, we find: 𝐹@788 = (100 𝑙𝑏)(sin 30°) = 50 𝑙𝑏 We now have both the horizontal and vertical components for the 100 − 𝑁 force. We will now do the same process for the other two forces acting on the system.



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The next force we will break up into components is the 50 𝑙𝑏 force. The angle at which the force is acting is not given, but we are given the side of a triangles. We can use trigonometric ratios to calculate each of the components.

Solving for the horizontal component of the force, we find:

𝐹6D8 = 𝐹 cos 𝜃 = (−50 𝑙𝑏)

4 = −40 𝑙𝑏 5

Solving for the vertical component of the force, we find:

𝐹@D8 = 𝐹 sin 𝜃 = (50 𝑙𝑏)



3 = 30 𝑙𝑏 5

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Next, the 80 𝑙𝑏 force acts with an opposite sense but similar angle relative to the origin, given as 𝜃 = 20°. We can then use this angle to determine the components.

Solving for the horizontal component of the force, we find: 𝐹6F8 = 𝐹 sin 𝜃 = (−80 𝑙𝑏)(sin 20°) = −27.36 𝑙𝑏 Solving for the vertical component of the force, we find: 𝐹@F8 = 𝐹 cos 𝜃 = (−80 𝑙𝑏)(cos 20°) = −75.17 𝑙𝑏



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As we know have the horizontal and vertical components of all the forces, we will sum the components to calculate the resultant of the forces in each component. Once we have the resultant of each component, we can use the formula to calculate the net resultant for the force for a 2-dimensional force system. Summing the horizontal component of each force, we find the net resultant force the horizontal component is: 𝐹6 = 𝐹6788 + 𝐹6D8 + 𝐹6F8 = 86.6 − 40 − 27.36 = 19.24 𝑙𝑏 Summing the vertical component of each force, we find the net resultant force the vertical component is:

𝐹@ = 𝐹@788 + 𝐹@D8 + 𝐹@F8 = 50 + 30 − 75.17 = 4.83 𝑙𝑏

The formula for the RESULTANT OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing. The RESULTANT or magnitude of the force (𝐹) of “𝑛” forces with components 𝐹6 ,K 𝑎𝑛𝑑 𝐹@ has the magnitude of: ,K

P

M

𝐹=

𝐹6 ,K KNO



P

M

+

𝐹@ KNO

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,K

P

M

=

𝐹6 ,K KNO

P

M

+

𝐹@ KNO

O P

,K

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Plugging in our calculated values for the resultant of the horizontal and vertical components, we find the net resultant of the forces acting on the hook to be:

𝐹=

19.24

P

+ 4.83

P

= 19.83 𝑙𝑏

The formula for the RESULTANT DIRECTION OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing. We then need to determine the angle that the force is acting at relative to the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠. The RESULTANT DIRECTION with respect to the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 is calculated as the arctangent of the ratio of the vertical component to the horizontal component:

𝜃 = arctan

M KNO 𝐹@ ,K M KNO 𝐹6 ,K

Plugging in our calculated values for the resultant of the horizontal and vertical components, we find the resultant direction of the forces acting on the hook to be:

𝜃 = arctan

4.83 = 14.09° 19.24

Therefore, the correct answer choice is A. 𝟏𝟗. 𝟖𝟑 𝒍𝒃; 𝟏𝟒. 𝟎𝟗°



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PROBLEM 2: A force system is shown below, what is the resultant magnitude and resultant direction of the three forces?

A. 45.29 𝑙𝑏; 22.22° B. 45.29 𝑙𝑏; 67.76° C. 53.10 𝑙𝑏; 33.09° D. 53.10 𝑙𝑏; 43.09°



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SOLUTION 2: The topic of the RESULTANT OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing.

This problem requires us to break each individual force up into components, sum them together, and then plug those components into the formula to calculate the resultant. The first step in this problem is to define our coordinate system. When working with two-dimensional problems, it is typical to use a Cartesian Coordinate System such that the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 represents the horizontal component, and the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 represents the vertical component.



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The next step is to cycle through each individual force, one at a time, and break the force into its horizontal and vertical components. We will start with the 120 𝑙𝑏 force highlighted in red.



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The line of action of the force is provided, as well as the sense of the angle relative to the origin, and is given as 40°. We can then use this angle to determine the components.

We will use trigonometric identities to solve for each of the components. We can identify the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 as our adjacent side, đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 as our opposite side, and the force vector as our hypotenuse.



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Calculating the horizontal component, we use the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 to represent the horizontal component of the force. Solving for the horizontal component of the force, we find: 𝐹67\8 = (120 𝑙𝑏)(cos 40°) = 91.93 𝑙𝑏 Moving on to the vertical component, we use the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 to represent the vertical component of the force.

Solving for the vertical component of the force, we find: 𝐹@7\8 = (120 𝑙𝑏)(sin 40°) = 77.13 𝑙𝑏 We now have both the horizontal and vertical components for the 120 𝑙𝑏 force. We will now do the same process for the other two forces acting in the system.



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The next force we will break up into components is the 60 𝑙𝑏 force. The angle at which the force is acting, is not given explicitly, but since the force is acting in only one direction we can determine its components easily. As the force acts at an angle on the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠, the force has a horizontal component of 0, as the force has only a vertical component.

Solving for the horizontal component of the force, we find: 𝐹6]8 = 0 𝑙𝑏 Solving for the vertical component of the force, we find: 𝐹@]8 = 60 𝑙𝑏

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The last force we will break up into components is the 130 𝑙𝑏 force. The angle at which the force is acting is not given, but we are given the side of a triangles. We can use trigonometric ratios to calculate each of the components.

Solving for the horizontal component of the force, we find:

𝐹67^8 = 𝐹 cos 𝜃 = (−130 𝑙𝑏)

5 = −50 𝑙𝑏 13

Solving for the vertical component of the force, we find:

𝐹@7^8 = 𝐹 sin 𝜃 = (−130 𝑙𝑏)



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12 = −120 𝑙𝑏 13

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As we now have the horizontal and vertical components of all the forces, we will sum the forces to calculate the resultant of the forces in each component. Once we have the resultant of each component, we can use the formula to calculate the net resultant for the force for a 2-dimensional force system. Summing the horizontal component of each force, we find the net resultant force the horizontal component is:

𝐹6 = 𝐹67\8 + 𝐹6]8 + 𝐹67^8 = 91.93 + 0 − 50 = 41.93 𝑙𝑏

Summing the vertical component of each force, we find the net resultant force the vertical component is:

𝐹@ = 𝐹@7\8 + 𝐹@]8 + 𝐹@7^8 = 77.13 + 60 − 120 = 17.13 𝑙𝑏 The formula for the RESULTANT OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing. The RESULTANT or magnitude of the force, 𝐹, of 𝑛 forces with components 𝐹6 ,K 𝑎𝑛𝑑 𝐹@ has the magnitude of:

P

M

𝐹=

𝐹6 ,K KNO



P

M

+

𝐹@ KNO

Made with

,K

P

M

=

𝐹6 ,K KNO

P

M

+

𝐹@ KNO

O P

,K

by Prepineer | Prepineer.com

,K

Plugging in our calculated values for the resultant of the horizontal and vertical components, we find the net resultant of the forces acting on the hook to be:

𝐹=

41.93

P

+ 17.13

P

= 45.29 𝑙𝑏

The formula for the RESULTANT DIRECTION OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing. We then need to determine the angle that the force is acting at relative to the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠. The RESULTANT DIRECTION with respect to the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 is calculated as the arctangent of the ratio of the vertical component to the horizontal component:

𝜃 = arctan

M KNO 𝐹@ ,K M KNO 𝐹6 ,K

Plugging in our calculated values for the resultant of the horizontal and vertical components, we find the resultant direction of the forces acting on the hook to be:

𝜃 = arctan

17.13 = 22.22° 41.93

Therefore, the correct answer choice is A. 𝟒𝟓. 𝟐𝟗 𝒍𝒃; 𝟐𝟐. 𝟐𝟐°



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PROBLEM 3: Using the free-body diagram of point C provided below, the sum of the forces along the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 is represented by which of the following expressions?

A. 𝐹P sin 50° − 20 = 0 B. 𝐹P cos 50° − 20 = 0 C. 𝐹P sin 50° − 𝐹O = 0 D. 𝐹P cos 50° + 20 = 0



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SOLUTION 3: The topic of the RESULTANT OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing. The first step in this problem is to define our coordinate system. When working with two-dimensional problems, it is typical to use a Cartesian Coordinate System such that the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 represents the horizontal component, and the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 represents the vertical component.

As we are simply looking for an expression to represent the sum of the forces about the x-axis, we can sum the force to write the expression: ∑𝐹6 = 0: 𝐹P cos 50° − 20 = 0

Therefore, the correct answer choice is B. 𝑭𝟐 𝒄𝒐𝒔 𝟓𝟎° − 𝟐𝟎 = 𝟎

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PROBLEM 4: Using the free-body diagram of point C provided below, the sum of the forces along the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 is represented by which of the following expressions?

A. 𝐹P sin 50° − 20 = 0 B. 𝐹P cos 50° − 20 = 0 C. 𝐹P sin 50° − 𝐹O = 0 D. 𝐹P cos 50° + 20 = 0



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SOLUTION 4: The topic of the RESULTANT OF A FORCE can be referenced under the topic of STATICS on page 67 of the NCEES Supplied Reference Handbook, 9.4 Version for Computer Based Testing. The first step in this problem is to define our coordinate system. When working with two-dimensional problems, it is typical to use a Cartesian Coordinate System such that the đ‘Ĩ − 𝑎đ‘Ĩ𝑖𝑠 represents the horizontal component, and the đ‘Ļ − 𝑎đ‘Ĩ𝑖𝑠 represents the vertical component.

As we are simply looking for an expression to represent the sum of the forces about the y-axis, we can sum the force to write the expression: ∑𝐹@ = 0: 𝐹P sin 50° − 𝐹O = 0

Therefore, the correct answer choice is C. 𝑭𝟐 𝒔𝒊𝒏 𝟓𝟎° − 𝑭𝟏 = 𝟎

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