Box sliding down an inclined plane

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SUMMARY

The discussion focuses on analyzing the motion of a box sliding down an inclined plane with no friction, involving two masses: the box (m1) and the inclined plane (m2). The key equations derived from Newton's laws include the contact forces (N1 and N2) and the accelerations of both the box and the inclined plane. The relationship between the accelerations is established through the equation involving the angle of inclination (θ), leading to the conclusion that the acceleration of the box relative to the inclined plane must align with the direction of the incline.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with inclined plane physics
  • Basic knowledge of vector decomposition
  • Ability to solve systems of equations
NEXT STEPS
  • Study the derivation of equations of motion for inclined planes
  • Learn about frictionless motion dynamics
  • Explore vector analysis in physics
  • Investigate the effects of varying angles of inclination on acceleration
USEFUL FOR

Students studying classical mechanics, physics educators, and anyone interested in understanding the dynamics of objects on inclined planes.

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Homework Statement

A box is placed on an inclined plane of angle [tex]\theta[/tex]. There is no fiction between the box and the plane nor between the inclined plane and the floor. The mass of the box is [tex]m_1[/tex] and the mass of the inclined plane is [tex]m_2[/tex].

Find the acceleration of the box and that of the inclined plane.


The attempt at a solution

It is easy to write down Newton's equations for both the box and the inclined plane.
Here they are:

[tex]N_1 \sin \theta = m_1 a_{1x}[/tex]

[tex]N_1 \cos \theta - m_1 g = m_1 a_{1y}[/tex]

[tex]- N_1 \sin \theta = m_2 a_{2x}[/tex]

[tex]N_2 - N_1 \cos \theta - m_2 g = 0[/tex]

where [tex]N_1[/tex] is the contact force between the box and the inclined plane and [tex]N_2[/tex] is the contact force between the inclined plane and the floor.

These are four equations in the unknowns [tex]N_1, N_2, a_{1x}, a_{1y}, a_{2x}[/tex].

How am I supposed to solve them?

My idea is the following: since the box is sliding down the inclined plane, the motion with respect to the inclined plane is easier. I mean the acceleration of the box relative to the inclined plane must be in the direction of the inclined plane. That is, the vector

[tex]\vec{a}_{box/plane} = \vec{a}_{box} - \vec{a}_{plane}[/tex]

should be in the direction of the plane. Thus

[tex]\tan \theta = \frac{a_{box/plane,y}}{a_{box/palne,x}} = \frac{a_{box,y}-a_{plane,y}}{a_{box,x}-a_{plane,x}} = \frac{a_{1y}}{a_{1x}-a_{2x}}.[/tex]

Is that right?
 
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