Is Acceleration Constant on an Inclined Plane?

AI Thread Summary
The acceleration of a cart rolling down an inclined plane is constant, assuming no resistances and a fixed angle. This acceleration is determined by the sine of the incline angle, which relates to gravity. As the angle increases, the acceleration also increases, following the formula a = g * sin(θ). The discussion emphasizes the importance of understanding the relationship between the incline angle and the gravitational force acting on the cart. Overall, the acceleration remains constant under ideal conditions, highlighting the principles of physics involved in inclined plane motion.
wallpaper
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Consider the system of a cart rolling down an inclined plane.

Is the acceleration constant? Why?
 
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Yes the acceleration is constant assuming no resistances and the incline is at a constant angle.

The acceleration vector of the cart is equal to the sine of the angle to the horizontal made by the incline. Since the angle and gravity are constant, the acceleration of the cart is also constant.
My reasoning as to why may only be intuitive though.
 
Ooh thanks. I have another question though, how does the degree of the tilt affect the acceleration?
 
wallpaper said:
Ooh thanks. I have another question though, how does the degree of the tilt affect the acceleration?

Like it was said:

Mentallic said:
The acceleration vector of the cart is equal to the sine of the angle to the horizontal made by the incline.
 
wallpaper said:
Ooh thanks. I have another question though, how does the degree of the tilt affect the acceleration?

I'll be a little more clear here :smile:

What you need to do is draw a diagram of the situation, labelling the angle \theta and the gravity acceleration vector (pointed directly towards the floor with a value of 9.8ms-2 if this scenario is on Earth's surface).
Now, what you need to find is the acceleration vector of the cart. This is simply the hypotenuse of your right-angled triangle that you were able to illustrate with the vectors. Since you have the angle, the opposite side and the hypotenuse; the relationship is:

sin\theta=\frac{opp}{hyp}

sin\theta=\frac{g}{a_f}
where:
af being the accleration of the cart
g=acceleration due to gravity

Therefore, a_f=\frac{g}{sin\theta}
 
The acceleration is

g*sin(theta)

where theta is the angle of the incline.
This is assuming no friction, of course.
If it were g/sin(theta) you'll get infinite acceleration on a horizontal plane...
 
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Yes your logical thinking sounds much more correct. However, this simple trigonometry is confusing me because I can't get that result. Can anyone spot my mistake?
 
Mentallic said:
Now, what you need to find is the acceleration vector of the cart. This is simply the hypotenuse of your right-angled triangle that you were able to illustrate with the vectors.
What you are trying to find is the component of g parallel to the incline, so g should be the hypotenuse of your triangle.
 

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