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(Figure 1)Block 1, of mass m1 = 0.700 kg , is connected over an ideal (massless and frictionless) pulley to block 2, of mass m2, as shown. For an angle of θ = 30.0 ∘ and a coefficient of kinetic friction between block 2 and the plane of μ = 0.400, an acceleration of magnitude a= 0.600 m/s2 is observed for block 2. Find the mass of block 2, m2

(Figure 1)Block 1, of mass m1 = 0.700 kg , is connected over an ideal (massless and frictionless) pulley to block 2, of mass m2, as shown. For an angle of θ = 30.0 ∘ and a coefficient of kinetic friction between block 2 and the plane of μ = 0.400, an acceleration of magnitude a= 0.600 m/s2 is observed for block 2. Find the mass of block 2, m2

College Physics
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
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(Figure 1)Block 1, of mass m1 = 0.700 kg , is connected over an ideal (massless and frictionless) pulley to block 2, of mass m2, as shown. For an angle of θ = 30.0 ∘ and a coefficient of kinetic friction between block 2 and the plane of μ = 0.400, an acceleration of magnitude a= 0.600 m/s2 is observed for block 2.

Find the mass of block 2, m2

### Description of the Diagram The image illustrates a physics problem involving a pulley system with two masses and an inclined plane. #### Components: 1. **Mass \( m_1 \)**: - Located on the left side, hanging vertically. - Connected to a pulley by a rope. - Experiences an acceleration \( \vec{a} \) directed downwards. 2. **Pulley**: - Positioned at the top left corner. - Assumes to be frictionless for theoretical simplicity. 3. **Mass \( m_2 \)**: - Positioned on the inclined plane. - Connected to the same rope and pulley as \( m_1 \). - Experiences an acceleration \( \vec{a} \) directed up the incline. 4. **Inclined Plane**: - Angled at \( \theta \) degrees relative to the horizontal base. - Has a coefficient of friction \( \mu \) with mass \( m_2 \). #### Forces and Motion: - Both masses are subject to gravitational forces. - Mass \( m_2 \) slides on the inclined plane with friction taken into account. - The acceleration \( \vec{a} \) shown on both masses indicates the direction of motion. - Mass \( m_1 \) is influenced by gravitational pull contributing to its downward motion. #### Analysis Context: To solve this system, we typically apply Newton's second law to each mass, considering forces such as tension in the rope, gravitational force, normal force, and friction on the inclined plane. The angle \( \theta \) and the coefficient \( \mu \) are crucial for determining the net forces and subsequent acceleration of the masses.
Transcribed Image Text:### Description of the Diagram The image illustrates a physics problem involving a pulley system with two masses and an inclined plane. #### Components: 1. **Mass \( m_1 \)**: - Located on the left side, hanging vertically. - Connected to a pulley by a rope. - Experiences an acceleration \( \vec{a} \) directed downwards. 2. **Pulley**: - Positioned at the top left corner. - Assumes to be frictionless for theoretical simplicity. 3. **Mass \( m_2 \)**: - Positioned on the inclined plane. - Connected to the same rope and pulley as \( m_1 \). - Experiences an acceleration \( \vec{a} \) directed up the incline. 4. **Inclined Plane**: - Angled at \( \theta \) degrees relative to the horizontal base. - Has a coefficient of friction \( \mu \) with mass \( m_2 \). #### Forces and Motion: - Both masses are subject to gravitational forces. - Mass \( m_2 \) slides on the inclined plane with friction taken into account. - The acceleration \( \vec{a} \) shown on both masses indicates the direction of motion. - Mass \( m_1 \) is influenced by gravitational pull contributing to its downward motion. #### Analysis Context: To solve this system, we typically apply Newton's second law to each mass, considering forces such as tension in the rope, gravitational force, normal force, and friction on the inclined plane. The angle \( \theta \) and the coefficient \( \mu \) are crucial for determining the net forces and subsequent acceleration of the masses.
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