Math Problem Statement

Block 1, of mass m1 = 0.650 kg, is connected over an ideal (massless and frictionless) pulley to block 2, of mass m, as shown. For an angle of θ = 30.0 and a coefficient of kinetic friction between block 2 and the plane of μ= 0.250, an acceleration of magnitude a = 0.400 m/s2 is observed for block 2. What is the mass of block 2?

Solution

To determine the mass m2m_2 of block 2, let's analyze the forces acting on both blocks and use Newton’s Second Law.

Step 1: Define the forces acting on both blocks

Block 1 (Hanging mass, m1m_1)

  • Weight: W1=m1gW_1 = m_1 g
  • Tension in the string: TT
  • Newton's Second Law:
    m1gT=m1am_1 g - T = m_1 a

Block 2 (on an inclined plane, m2m_2)

  • Weight components:
    • Perpendicular to the plane: m2gcosθm_2 g \cos\theta
    • Parallel to the plane: m2gsinθm_2 g \sin\theta
  • Kinetic friction force:
    fk=μm2gcosθf_k = \mu m_2 g \cos\theta
  • Tension in the string: TT
  • Newton's Second Law along the plane: Tfkm2gsinθ=m2aT - f_k - m_2 g \sin\theta = m_2 a

Step 2: Express Tension TT from Block 1

From the equation for Block 1: T=m1gm1aT = m_1 g - m_1 a

Step 3: Substitute TT into Block 2's equation

(m1gm1a)(μm2gcosθ)(m2gsinθ)=m2a(m_1 g - m_1 a) - (\mu m_2 g \cos\theta) - (m_2 g \sin\theta) = m_2 a

Step 4: Solve for m2m_2

m1gm1aμm2gcosθm2gsinθ=m2am_1 g - m_1 a - \mu m_2 g \cos\theta - m_2 g \sin\theta = m_2 a

Factor out m2m_2: m1gm1a=m2g(μcosθ+sinθ)+m2am_1 g - m_1 a = m_2 g (\mu \cos\theta + \sin\theta) + m_2 a

m2(g(μcosθ+sinθ)+a)=m1gm1am_2 (g (\mu \cos\theta + \sin\theta) + a) = m_1 g - m_1 a

m2=m1gm1ag(μcosθ+sinθ)+am_2 = \frac{m_1 g - m_1 a}{g (\mu \cos\theta + \sin\theta) + a}

Step 5: Plug in Values

  • m1=0.650m_1 = 0.650 kg
  • g=9.81g = 9.81 m/s²
  • a=0.400a = 0.400 m/s²
  • θ=30.0\theta = 30.0^\circ
  • μ=0.250\mu = 0.250

Calculate the denominator: g(μcosθ+sinθ)+a=9.81(0.250cos30+sin30)+0.400g (\mu \cos\theta + \sin\theta) + a = 9.81 (0.250 \cos 30^\circ + \sin 30^\circ) + 0.400

=9.81(0.250×0.866+0.5)+0.400= 9.81 (0.250 \times 0.866 + 0.5) + 0.400

=9.81(0.2165+0.5)+0.400= 9.81 (0.2165 + 0.5) + 0.400

=9.81×0.7165+0.400= 9.81 \times 0.7165 + 0.400

=7.0265+0.400= 7.0265 + 0.400

=7.4265= 7.4265

Calculate the numerator: m1gm1a=(0.650×9.81)(0.650×0.400)m_1 g - m_1 a = (0.650 \times 9.81) - (0.650 \times 0.400)

=6.37650.26= 6.3765 - 0.26

=6.1165= 6.1165

Now solve for m2m_2:

m2=6.11657.4265m_2 = \frac{6.1165}{7.4265}

m20.824 kgm_2 \approx 0.824 \text{ kg}

Final Answer:

0.824 kg\boxed{0.824 \text{ kg}}

Would you like a deeper breakdown of any part of the solution?

Related Questions:

  1. What would happen if the coefficient of friction were increased?
  2. How would the acceleration change if the angle θ\theta was steeper?
  3. What if the masses were equal—how would the system behave?
  4. How does the tension in the rope change with different masses?
  5. What is the normal force acting on block 2?

Tip:

In inclined plane problems, always resolve forces into components parallel and perpendicular to the surface—it simplifies calculations significantly. 🚀

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Math Problem Analysis

Mathematical Concepts

Newton's Second Law
Kinematics
Friction
Inclined Plane Physics

Formulas

Newton's Second Law: F = ma
Tension in rope: T = m1 g - m1 a
Kinetic friction force: f_k = μ m2 g cosθ
Force equation along the plane for block 2: T - f_k - m2 g sinθ = m2 a

Theorems

Newton's Second Law of Motion
Inclined Plane Mechanics
Frictional Forces on Inclined Planes

Suitable Grade Level

Grades 11-12