4.31 System Chapter 11 we are much smarter and are able to show that for a c m, the force required to deflect the end, as is illustrated in Figure 4.32 is F = 4.32 Cantilever beam subjected to a at the end. ЗЕЛ L3 buieds x=0 cantilever F-XX ere E is the modulus of elasticity, which is a property of the material used, I is area moment of inertia of the cross-section of the beam, and L is the length. fa mass m,is attached to the end of the beam, what is the equation of motion the vertical motion of the beam? If the length is doubled, what is the change in uency of the free vibration of the beam? jaký F x=L
4.31 System Chapter 11 we are much smarter and are able to show that for a c m, the force required to deflect the end, as is illustrated in Figure 4.32 is F = 4.32 Cantilever beam subjected to a at the end. ЗЕЛ L3 buieds x=0 cantilever F-XX ere E is the modulus of elasticity, which is a property of the material used, I is area moment of inertia of the cross-section of the beam, and L is the length. fa mass m,is attached to the end of the beam, what is the equation of motion the vertical motion of the beam? If the length is doubled, what is the change in uency of the free vibration of the beam? jaký F x=L
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
Problem 1.1MA
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![### Understanding Cantilever Beam Deflection
#### Theory and Equation
In this section, we explore the concept of cantilever beam deflection. A cantilever beam is fixed at one end and free at the other, and the beam bends when a force is applied at the free end.
The formula to calculate the force \( F \) required to deflect the end of a cantilever beam is given as:
\[
F = \frac{3EI}{L^3} x
\]
Where:
- \( E \) is the modulus of elasticity of the material.
- \( I \) is the area moment of inertia of the beam's cross-section.
- \( L \) is the length of the beam.
- \( x \) is the deflection of the beam at the end.
#### Diagram Explanation
The diagram (Figure 4.32) shows a cantilever beam subjected to a force at its free end:
- The beam is horizontally positioned, fixed at \( x = 0 \) and free at \( x = L \).
- The beam is bending due to the force \( F \) applied at \( x = L \).
#### Problem Statements
1. If a mass \( m \) is attached to the end of the beam, determine the equation of motion for the vertical motion of the beam.
2. If the length of the beam is doubled, analyze the effect on the frequency of the free vibration of the beam.
This conceptual understanding aids in predicting the behavior of materials under stress, vital for fields such as structural engineering and materials science.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F018b6ab2-59a7-41b6-bb67-75e1f30a7b02%2Fd38b00db-e6eb-4033-98a4-e5d285696d28%2Fv0q8dt_processed.jpeg&w=3840&q=75)
Transcribed Image Text:### Understanding Cantilever Beam Deflection
#### Theory and Equation
In this section, we explore the concept of cantilever beam deflection. A cantilever beam is fixed at one end and free at the other, and the beam bends when a force is applied at the free end.
The formula to calculate the force \( F \) required to deflect the end of a cantilever beam is given as:
\[
F = \frac{3EI}{L^3} x
\]
Where:
- \( E \) is the modulus of elasticity of the material.
- \( I \) is the area moment of inertia of the beam's cross-section.
- \( L \) is the length of the beam.
- \( x \) is the deflection of the beam at the end.
#### Diagram Explanation
The diagram (Figure 4.32) shows a cantilever beam subjected to a force at its free end:
- The beam is horizontally positioned, fixed at \( x = 0 \) and free at \( x = L \).
- The beam is bending due to the force \( F \) applied at \( x = L \).
#### Problem Statements
1. If a mass \( m \) is attached to the end of the beam, determine the equation of motion for the vertical motion of the beam.
2. If the length of the beam is doubled, analyze the effect on the frequency of the free vibration of the beam.
This conceptual understanding aids in predicting the behavior of materials under stress, vital for fields such as structural engineering and materials science.
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