Diff Eqs for a block moving sideways down a plane

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SUMMARY

The discussion focuses on the dynamics of a block moving down an inclined plane, initially kicked with speed V perpendicular to the slope. The key conclusion is that the speed of the block down the plane after a long time, given a coefficient of friction of tan θ, is V/2. The equations of motion derived include -mg sin θ cos γ = m ¨x and mg sin θ - mg sin θ sin γ = m ¨y, leading to the simplification of these equations to express the relationship between the velocities and accelerations in both directions. The total speed is confirmed to be constant, with the relationship √(v_x² + v_y²) + v_y = C.

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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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