Two blocks connected by string on inclined plane — find acceleration and tension

easy CBSE JEE-MAIN NEET 3 min read

Question

Two blocks of masses m1=5m_1 = 5 kg and m2=3m_2 = 3 kg are connected by a light string over a frictionless pulley at the top of a frictionless inclined plane (angle 30°). m1m_1 hangs vertically and m2m_2 is on the inclined surface. Find the acceleration of the system and tension in the string. (g = 10 m/s²)

Solution — Step by Step

The system consists of:

  • m1=5m_1 = 5 kg: Hanging freely, weight m1g=50m_1 g = 50 N downward
  • m2=3m_2 = 3 kg: On incline (30°), weight m2g=30m_2 g = 30 N vertically downward

Assume m1m_1 moves down (and m2m_2 moves up the incline) — take this as positive direction.

Forces on m1m_1: weight m1gm_1g downward, tension TT upward.

m1gT=m1am_1g - T = m_1 a 50T=5a...(1)50 - T = 5a \quad ...(1)

Forces on m2m_2 along the incline:

  • Component of weight down the incline: m2gsin30°=30×0.5=15m_2 g\sin 30° = 30 \times 0.5 = 15 N (opposing upward motion)
  • Tension TT up the incline (pulling it up)

Net force on m2m_2 up the incline = Tm2gsinθT - m_2g\sin\theta

Tm2gsin30°=m2aT - m_2g\sin 30° = m_2 a T15=3a...(2)T - 15 = 3a \quad ...(2)

Add equations (1) and (2):

(50T)+(T15)=5a+3a(50 - T) + (T - 15) = 5a + 3a 35=8a35 = 8a a=358=4.375 m/s24.4 m/s2a = \frac{35}{8} = 4.375 \text{ m/s}^2 \approx 4.4 \text{ m/s}^2

Substitute back into (2):

T=15+3×4.375=15+13.125=28.125 N28.1 NT = 15 + 3 \times 4.375 = 15 + 13.125 = 28.125 \text{ N} \approx 28.1 \text{ N}

From (1): 50T=5a=5×4.375=21.87550 - T = 5a = 5 \times 4.375 = 21.875

T=5021.875=28.125T = 50 - 21.875 = 28.125 N ✓

Answer: Acceleration = 4.4 m/s², Tension = 28.1 N

Why This Works

The two blocks are connected by an inextensible string, so they have the same magnitude of acceleration. By applying Newton’s 2nd law to each block separately and adding the equations, the unknown tension cancels, giving us acceleration directly.

The inclined plane problem reduces to a simpler form because the surface is frictionless. Only the component of gravity along the incline (m2gsinθm_2 g\sin\theta) acts as resistance; the normal force (m2gcosθm_2 g\cos\theta) is balanced by the surface’s normal reaction and plays no role in acceleration.

General formula for this type of problem: when mass m1m_1 hangs vertically and mass m2m_2 is on an incline at angle θ\theta (frictionless):

a=m1gm2gsinθm1+m2=(m1m2sinθ)gm1+m2a = \frac{m_1 g - m_2 g\sin\theta}{m_1 + m_2} = \frac{(m_1 - m_2\sin\theta)g}{m_1 + m_2}

Substituting: a=(53×0.5)×108=3.5×108=4.375a = \frac{(5 - 3 \times 0.5) \times 10}{8} = \frac{3.5 \times 10}{8} = 4.375 m/s². Same answer, faster route once you derive the formula.

Common Mistake

Students frequently use the full weight m2gm_2 g for the inclined block instead of m2gsinθm_2 g\sin\theta. The full weight acts downward; only its component ALONG the incline opposes the string tension. The component perpendicular to the incline (m2gcosθm_2 g\cos\theta) is balanced by the normal force — it plays NO role in the motion along the incline. This is the most common error in Atwood-on-incline problems, and it gives a completely wrong answer.

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