Diff Eqs for a block moving sideways down a plane

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Homework Help Overview

The problem involves a block moving down an inclined plane after being kicked perpendicular to the slope with an initial speed V. The discussion centers around determining the block's speed down the plane after a long time, considering the coefficient of friction is equal to tan θ.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore different methods to analyze the motion of the block, including using equations of motion and considering the relationship between the components of velocity. There are attempts to derive equations for the acceleration in both the x and y directions, and questions arise about the assumptions regarding the constancy of total speed and the implications of the derived equations.

Discussion Status

Participants are actively questioning the assumptions made in the original post, particularly regarding the constancy of certain quantities. Some have provided alternative perspectives and references to similar problems, while others are attempting to clarify the relationships between the variables involved in the motion.

Contextual Notes

There is ongoing debate about the correctness of defining certain constants and the implications of the derived equations. Participants are also considering the effects of friction and the long-term behavior of the block's motion.

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Homework Statement


I was looking at the problem discussed in the thread below.
https://www.physicsforums.com/showthread.php?t=502417

A block is initially kicked in the direction perpendicular to the downslope of the plane with initial speed V.
The problem asks for the speed of the block down the plane after a long time if the coeff of friction is tan \theta.

Homework Equations



The thread I posted above mentions using the fact that \sqrt{v_x^2 + v_y^2} + v_y = C, where C is a constant, since the speed gained in the y-direction will be equal to the speed lost overall.

C is initially V. Eventually v_x goes to zero and v_y goes to v_f. So
v_f + v_f = V and the speed down the plane after a long period of time is \frac{V}{2}

However, I am interested if this problem can be solved in another way, using the equations of motion.

The Attempt at a Solution



If \gamma = arctan \frac{v_y}{v_x}, then the equations of motion for the x (perpendicular to the downslope) and y (down the slope) directions respectively will be

-mg\,sin\theta\, cos \gamma = m \ddot x
mg\,sin\theta - mg\,sin\theta\, sin\gamma = m \ddot y

These simplify to

\frac {-gsin\theta}{\sqrt{\frac{v_y^2}{v_x^2} + 1}} = \ddot x
gsin\theta \,(1-\frac{\frac{v_y}{v_x}}{\sqrt{\frac{v_y^2}{v_x^2} +1 }}) = \ddot y

Also, v_y = \dot y and v_x = \dot x. The total speed, V = v_y^2 + v_x^2, is constant too. So we further can further simplify the equations to these:

\frac{-gsin\theta}{V} \dot x = \ddot x
gsin\theta \,(1-\frac{\dot y}{V}) = \ddot y

I am wondering how to proceed in solving these equations. I am trying to find \dot y.
 
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joej24 said:
\frac{-gsin\theta}{V} \dot x = \ddot x
gsin\theta \,(1-\frac{\dot y}{V}) = \ddot y

I am wondering how to proceed in solving these equations. I am trying to find \dot y.

You can't take the next step algebraically and solve for \dot y?

Also, shouldn't The total speed be v^2 = v^2_y+v^2_x?
 
Right, the total speed should be v^2, not v. Then the square root makes it v.

Seperating the equation for \dot y,
\dot y \, = \, v \, (1 \, - \, \frac{\ddot y}{g\,sin\theta}).

As t -> \infty, \ddot y -> 0 because the block will be moving straight down the incline. This can't be correct though, because that would mean \dot y -> v.

Finding y(t) isn't as hard as I thought. I can integrate both sides of the motion equation to obtain v \,( t - \frac{\dot y}{g\,sin\theta}) = y + y_0. But we can say that y(0) = 0 to get rid of the y_0 term.

Then I rearrange the terms to get \dot y + (\frac {g\,sin\theta}{v}) \, y = (g\,sin\theta)\,t.
This is a first order linear diff eq that's solvable.

y = Ce^{-\frac{g\,sin\theta}{v} t} + e^{-\frac{g\,sin\theta}{v} t} \int (g\,sin\theta) \,t \, e^{\frac{g\,sin\theta}{v} t}

I simplified this down to
y = vt - \frac{v^2}{g\,sin\theta} + Ce^{\frac{-g\,sin\theta}{v}t}

So,

\dot y = v - \frac{g\,sin\theta}{v} C e^{\frac{-g\,sin\theta}{v}t}.

But, this also suggests that \dot y goes to v instead of \frac{v}{2}.
 
joej24 said:

Homework Statement


I was looking at the problem discussed in the thread below.
https://www.physicsforums.com/showthread.php?t=502417

A block is initially kicked in the direction perpendicular to the downslope of the plane with initial speed V.
The problem asks for the speed of the block down the plane after a long time if the coeff of friction is tan \theta.

2.

However, I am interested if this problem can be solved in another way, using the equations of motion.

The Attempt at a Solution



If \gamma = arctan \frac{v_y}{v_x}, then the equations of motion for the x (perpendicular to the downslope) and y (down the slope) directions respectively will be

-mg\,sin\theta\, cos \gamma = m \ddot x
mg\,sin\theta - mg\,sin\theta\, sin\gamma = m \ddot y

These simplify to

\frac {-gsin\theta}{\sqrt{\frac{v_y^2}{v_x^2} + 1}} = \ddot x
gsin\theta \,(1-\frac{\frac{v_y}{v_x}}{\sqrt{\frac{v_y^2}{v_x^2} +1 }}) = \ddot y

Also, v_y = \dot y and v_x = \dot x. The total speed, V = v_y^2 + v_x^2, is constant too.


Why should be the total speed constant?



ehild
 
I think the whole premiss that C as defined at the OP is a constant is just pain wrong. Why would that be the case?
 
ehild said:
Why should be the total speed constant?
ehild

That's a mistake. I realize now that total speed + v_y is a constant, \sqrt{v_x^2 + v_y^2} + v_y = C. I will check out the link you posted, which is the same problem, and try to redo my math.
 

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