Why Are the Two Angles Labeled Theta Equal?

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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


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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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##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!