Final answer:
By using conservation of energy and the negligible effects of air resistance and friction, the trolley's potential energy at point A is converted into kinetic energy at point B, leading to a final speed of about 3 m/s.
Step-by-step explanation:
Calculating the Speed of a Trolley at Point B
To show that the trolley reaches point B with a speed of about 3 m/s, we can use the principles of energy conservation. Since air resistance and friction are negligible, the mechanical energy of the trolley is conserved. We'll assume the potential energy of the trolley at point A is converted into kinetic energy at point B.
The potential energy at point A (PEA) is equal to the product of mass m, gravitational acceleration g (approximately 9.8 m/s²), and height h. The kinetic energy (KEB) at point B is ½mv², where v is the velocity at point B.
Using the formula: PEA = KEB, we get:
mgh = ½mv²
Since the mass m cancels out, we can solve for v:
gh = ½v²
Substituting g = 9.8 m/s² and h = 0.50 m gives:
(9.8 m/s²)(0.50 m) = ½v²
4.9 m²/s² = ½v²
v² = 9.8 m²/s²
v = √(9.8 m²/s²)
v ≈ 3.13 m/s
Thus, the trolley reaches point B with a speed of approximately 3.13 m/s, which is about 3 m/s.