Why Are the Two Angles Labeled Theta Equal?

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Homework Help Overview

The discussion revolves around understanding a figure in a statics textbook related to vector analysis and the moment of a force about a specific axis. The original poster is specifically questioning why two angles labeled theta in the figure are equal, with one angle being between the position vector and the x-axis, and the other between the moment and its y component.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the angles in question, with some attempting to clarify the geometric relationships and definitions involved in the moment of a force. Questions arise about the implications of complementary angles and the definitions of the moment and position vectors.

Discussion Status

The discussion is active, with participants providing clarifications and exploring the relationships between the angles. Some guidance has been offered regarding the complementary nature of the angles, but there remains a request for further clarification on why the angles labeled theta are equal.

Contextual Notes

Participants are working within the constraints of a textbook figure and the definitions provided in the context of statics and vector analysis. There is an emphasis on understanding the geometric relationships without providing a definitive solution.

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Homework Statement



In my statics book (13th ed. Hibbeler) I'm reviewing the section about using vector analysis to calculate the moment of a force about a specific axis. I understand the theory fine, but I don't completely understand the figure in the book (pic attached). Specifically, why are the two angles labeled theta equal? The first tangle is between the position vector and the x axis, and the second angle is between the moment and it's y component.

Homework Equations



Trig relations would obviously be of some help.

The Attempt at a Solution


[/B]
Since ##r## is any vector from point O extending to the line of action of the applied force, doesn't that mean we can adjust ##r## and still maintain the same moment ##M_O##? Thus ##\theta## between ##r## and the x-axis is changing while ##\theta## between ##M_O## and ##M_y## remains the same?
 

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What is Mo?
 
##M_O## is the moment of the force ##F## about the axis through point O.
 
OK. What is the direction of Mo in respect to the plane determined by F and r? What is the angle between Mo and r?
 
##M_O## is, by definition, perpendicular to the plane containing ##F## and ##r##. The angle between ##M_O## and ##r## is thus 90°.
 
Great. so now you see why the two angles are equal?
The angle between the y-axis and r should give 90 when added to theta, right?
 
Yes, but I don't exactly understand how the angle between the y-axis and ##r##, and the angle ##\theta## being complementary to one another tells us anything about the angle between ##M_O## and ##M_y##.

I get that the angles adjacent to ##\theta## are equivalent to ##90-\theta##, but, to me, that doesn't explain why both ##\theta##'s seem to be equal.

Can you please clarify?
 
If we call "alpha" the angle between r and My, it is complementary to both angles labeled "theta".
Or both angles have the same complementary angle (alpha).
 
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Thanks a ton, I got it now! Interesting way of looking at things!
 

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