A horse pulls a cart forward. According to Newton's third law, the cart pulls the horse backward with equal force. Why does the horse-cart system still accelerate forward?
Solution:
The horse-on-cart and cart-on-horse forces act on different bodies — they do not cancel on the system. Acceleration is determined by the net horizontal force on each body, which includes the friction the ground exerts on the horse.
Q6 — Tension (elevator)
A \(60\)-kg person stands on a scale in an elevator accelerating upward at \(2.0\) m/s². What is the scale reading (apparent weight)?
Answer: N
Solution:
\( N - mg = ma \) (upward positive). \( N = m(g+a) = 60(9.8+2.0) = 60(11.8) = 708 \) N
Q7 — Friction on incline
A \(10\)-kg block sits on a \(20°\) incline. The static friction coefficient is \(0.40\). Will it slide?
Solution:
\( F_\parallel = mg\sin(20°) = 10(9.8)(0.342) = 33.5 \) N
\( f_s^\text{max} = \mu_s mg\cos(20°) = 0.40(10)(9.8)(0.940) = 36.8 \) N
Since \( 33.5 < 36.8 \), static friction is sufficient — the block does not slide.
Q8 — Atwood machine
Two masses, \(3.0\) kg and \(5.0\) kg, hang from a frictionless pulley. What is the acceleration of the system?
A 2.0-kg block and a 3.0-kg block are pushed together on a frictionless surface by a horizontal force of \(20\) N applied to the 2.0-kg block. What is the contact force between them?
Answer: N
Solution:
System: \( a = 20/(2+3) = 4.0 \) m/s²
Force on 3.0-kg block: \( F = m_2 a = 3.0(4.0) = 12 \) N