IBDP Physics- A.2 Forces and momentum- IB Style Questions For HL Paper 1A -FA 2025
Question
(B) \(\frac{F \sin \theta – mg}{m}\)
(C) \(\frac{F \cos \theta – g}{m}\)
(D) \(\frac{F \sin \theta – g}{m}\)
▶️ Answer/Explanation
Resolving the force \( F \) into components:
– Vertical component: \( F \cos \theta \) (upwards)
– Horizontal component: \( F \sin \theta \) (perpendicular to the surface)
Since the surface is frictionless and vertical, only the vertical forces affect the upward acceleration.
Using Newton’s second law in the vertical direction:
\( F \cos \theta – mg = ma \)
Rearranging for acceleration \( a \):
\( a = \frac{F \cos \theta – mg}{m} \)
✅ Answer: (A)
Question
▶️ Answer/Explanation
The ball moves in a horizontal circle with constant speed.
Therefore, the vertical component of the tension balances the weight of the ball, so the net vertical force is zero.
The horizontal component of the tension provides the centripetal force required for the circular motion.
✅ Answer: (D)
Question
The trolley accelerates at a rate of \(1.0\,\text{m s}^{-2}\).
What is the coefficient of dynamic friction between the block and the trolley?
(B) \(0.15\)
(C) \(0.25\)
(D) \(0.35\)
▶️ Answer/Explanation
Since the trolley accelerates at \(1.0\,\text{m s}^{-2}\) and the friction with the ground is zero, the only horizontal force acting on the trolley is the friction force due to the block.
Hence, the friction force is \( F = ma = 5.0 \times 1.0 = 5.0\,\text{N} \).
The normal reaction between the block and the trolley is \( N = mg = 2.0 \times 10 = 20\,\text{N} \).
Using \( F = \mu_k N \), \( \mu_k \times 20 = 5.0 \).
Therefore, \( \mu_k = 0.25 \).
✅ Answer: (C)
