Component resolution of g on an inclined plane

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Homework Help Overview

The discussion revolves around the concept of gravitational acceleration (g) on an inclined plane, specifically how to experimentally determine g using the acceleration of an object moving down the ramp and trigonometric relationships. Participants are exploring the correct application of sine in relation to the angles involved in the setup.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are questioning the relationship between gravitational acceleration and the acceleration down the ramp, particularly the use of trigonometric functions to resolve components. There is a discussion on whether g can be expressed as a function of the ramp's acceleration and angle.

Discussion Status

Some participants have provided insights into the correct setup of triangles in the context of the problem, suggesting that the original poster may not have the correct understanding of the relationships between the sides of the triangle formed by the gravitational force and the acceleration down the ramp. There is an ongoing exploration of the implications of these relationships.

Contextual Notes

Participants are working within the constraints of a homework assignment, which may limit the information they can use or the methods they can apply. The discussion reflects a need for clarity on the geometric interpretation of forces involved in the problem.

themselv
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Homework Statement



Hi, I just had a quick conceptual question.
I understand that if I have an object moving down a ramp, it is being accelerated only by gravity. My question is this:

We should be able to experimentally calculate g if we measure the acceleration down the ramp. Then we can use trigonometry to determine a value for g. However, this only works if you take the
acceleration down the ramp divided by the sin (theta) . I understand where this comes from (redrawing the angle theta in the middle where the object starts from), but why can we not calculate the component of gravity by saying:

sin (theta) = g / a

This makes more sense to me looking at the initial angle, because g appears to be the opposite side and the acceleration down the ramp appears to be the hypotenuse.

Can someone please help clarify?



Homework Equations





The Attempt at a Solution

 
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themselv said:

Homework Statement



Hi, I just had a quick conceptual question.
I understand that if I have an object moving down a ramp, it is being accelerated only by gravity. My question is this:

We should be able to experimentally calculate g if we measure the acceleration down the ramp. Then we can use trigonometry to determine a value for g. However, this only works if you take the
acceleration down the ramp divided by the sin (theta) . I understand where this comes from (redrawing the angle theta in the middle where the object starts from), but why can we not calculate the component of gravity by saying:

sin (theta) = g / a

This makes more sense to me looking at the initial angle, because g appears to be the opposite side and the acceleration down the ramp appears to be the hypotenuse.

Can someone please help clarify?



Homework Equations





The Attempt at a Solution



I think it will be easier if you draw a diagram
 
pzqwWWV.png


I realize that an expression for g should be g = a/sin(theta) by looking at the angle that's formed perpendicular to the plane.

However, if I just look at angle theta in the bottom left corner, why am I not justified in saying g = sin(theta)*a, since to me it appears that the sine of angle theta is just opposite over hypotenuse, or g/a.
 
"However, if I just look at angle theta in the bottom left corner, why am I not justified in saying g = sin(theta)*a, since to me it appears that the sine of angle theta is just opposite over hypotenuse, or g/a."

Because you've not got the correct triangle set up. The hypoteneuse of a triangle is its longest side. The component of the gravitational acceleration (g) in the down incline direction is what gives you a. Since a component (a) can never exceed the full vector (g) in magnitude, it follows that a cannot be the hypoteneuse.

Chris.
 
The hypotenuse is the longest side, which is (correctly) labelled g in your diagram. The side opposite angle ## \theta ## is (correctly) labelled a. So opposite over hypotenuse is ## \frac{a}{g} ## not ## \frac{g}{a} ##.
 

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