Dynamic Equilibrium -- Acceleration of a rock thrown from a bridge

AI Thread Summary
The discussion clarifies that the only force acting on a rock in free fall, when air resistance is neglected, is the gravitational force, represented as mg, which causes the rock to accelerate at g. It emphasizes the distinction between forces and accelerations, noting that acceleration is not a force itself. When an object is thrown upward or downward, the acceleration remains constant at g, regardless of the initial velocity. Newton's laws are referenced to explain that the net force equals the gravitational force, leading to the conclusion that acceleration equals g. Visual aids, like force diagrams, are recommended for better understanding of these concepts.
Dman0500
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Homework Statement
A rock is thrown from a bridge at an angle 30° below horizontal. Immediately after the rock is released, is the magnitude of its acceleration greater than, less than, or equal to g? Explain.
Relevant Equations
Conceptual
I know the acceleration of the rock is equal to g, but why. If we neglect air resistance, what is actually making the rock fall? Wouldn't it be that g overcomes the acceleration of the y plane at some point so the rock starts coming down or in this case accelerate more by throwing below 0 degrees?
 
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What are forces on the rock?
 
I suppose just g and a(y-axis)
 
Dman0500 said:
I suppose just g and a(y-axis)

There is a weight force, of magnitude ##mg##, acting downward. That is the only force! "##a##" is not a force, it is an acceleration!

What is Newton's second law?
 
Alright I get it now!
alright so when something is thrown upward, there is still only g?
 
Dman0500 said:
Alright I get it now!
alright so when something is thrown upward, there is still only g?

Yes, something undergoing free-fall (only force is the gravitational ##m\vec{g}##) will accelerate at ##\vec{g}##. Make sure you are clear to distinguish forces from accelerations!

The result follows from Newton's first law; the net force is ##m\vec{g}##, and Newton tells us that ##m\vec{g} = m\vec{a}##. So ##\vec{a} = \vec{g}##.

If you throw something downward, it has an initial downward component of velocity. However the acceleration is still just ##\vec{g}##!
 
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Make way more sense thank you
 
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Likes berkeman and etotheipi
No problem. If you are ever in doubt about similar matters, draw a diagram! Draw the forces on the diagram, and then use ##\vec{F} = m\vec{a}##.
 
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