Particle Motion in a Vertical Plane: Trajectory Equation & Curve

In summary, a particle moves in a vertical plane from rest under the influence of gravity and a force perpendicular to and proportional to its velocity. The equation of the trajectory can be obtained by using the equations of motion and identifying the curve. At t=0, the particle has zero velocity and its position in the x and y direction is also zero.
  • #1
lfdahl
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A particle moves in a vertical plane from rest under the influence of gravity
and a force perpendicular to and proportional to its velocity. Obtain the equation of the
trajectory, and identify the curve.
 
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  • #2
Hint:

The equations of motion are:

\[m\ddot{y} = mg-k\dot{x},\: \: \: m\ddot{x} = k\dot{y}\]

One dot means a differentiation with respect to t (time): $\frac{dy}{dt} = \dot{y}.$
 
  • #3
Suggested solution:

Assume the mass is dropped from $x=y=0$ at $t=0$. Let the $y$-axis be positive down. We then have:
(Force = k velocity and physics notation: $\dot{y} = \frac{dy}{dt}$)

\[m\ddot{y} = mg-k\dot{x},\: \: \: m\ddot{x} = k\dot{y}\]

Or
\[\ddot{y} = g-w\dot{x},\: \: \: \ddot{x} = w\dot{y},\: \: \: w = k/m.\]

Substituting gives: \[\frac{\mathrm{d}^2\dot{y} }{\mathrm{d} t^2} =-w^2\dot{y}\]

Or

\[\dot{y} = B \sin (wt)\Rightarrow y = -\frac{B}{w}\cos (wt)+\frac{B}{w} \\\\ \dot{x}=-B\cos (wt)+B \Rightarrow x = -\frac{B}{w} \sin (wt)+Bt\]
Substitution in original differential equation gives: $B = g/w$.

Finally

\[x = -\frac{g}{w^2} \sin (wt)+\frac{g}{w}t \\\\ y = -\frac{g}{w^2}\cos (wt)+\frac{g}{w^2}\]

These determine a cycloid produced by a wheel of radius $R = g/w^2$ rolling on the $x$-axis at speed $\frac{g}{w}$, where $w = k/m$.
 
  • #4
lfdahl said:
A particle moves in a vertical plane from rest under the influence of gravity
and a force perpendicular to and proportional to its velocity. Obtain the equation of the
trajectory, and identify the curve.

Since the particle moves from rest shouldn't we have : at t=0 ,dy/dt=dx/dt=x=y=0 ??
 
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  • #5
solakis said:
Since the particle moves from rest shouldn't we have : at t=0 ,dy/dt=dx/dt=x=y=0 ??
Yes, and as far as I can see, these conditions are fulfilled:

\[\dot{x}(0) = -\frac{g}{w}\cos (0)+\frac{g}{w} = 0 \\\\ \dot{y} = \frac{g}{w}\sin (0) =0\]

Likewise:

$x(0) = y(0) = 0$.
 
  • #6
lfdahl said:
Hint:

The equations of motion are:

\[m\ddot{y} = mg-k\dot{x},\: \: \: m\ddot{x} = k\dot{y}\]

One dot means a differentiation with respect to t (time): $\frac{dy}{dt} = \dot{y}.$

I would like to know how you got the equations of motion ,if it is possible

Thanks
 
  • #7
solakis said:
I would like to know how you got the equations of motion ,if it is possible

Thanks
The two only forces involved in the cycloid motion are the gravitational force, and a velocity dependent force.
The former is in our coordinate system simply:

\[\vec{F_g} = m\binom{0}{g}\]

The latter force is proportional to the particle velocity, $\vec{v}= \binom{\dot{x}}{\dot{y}}$, and perpendicular to it. Hence we have:

\[\boldsymbol{F}_v = -k \hat{\mathbf{v}} = -k\binom{-\dot{y}}{\dot{x}} = k\binom{\dot{y}}{-\dot{x}}\]

Using Newtons 2nd law:

\[\boldsymbol{F}_{res} = m\binom{\ddot{x}}{\ddot{y}} = \boldsymbol{F}_g + \boldsymbol{F}_v = m\binom{0}{g} +k\binom{\dot{y}}{-\dot{x}}\]

In component form:

\[m\ddot{x} = k\dot{y}\\\\ m\ddot{y} = mg - k \dot{x}\]
 
  • #8
lfdahl said:
The two only forces involved in the cycloid motion are the gravitational force, and a velocity dependent force.
The former is in our coordinate system simply:

\[\vec{F_g} = m\binom{0}{g}\]

The latter force is proportional to the particle velocity, $\vec{v}= \binom{\dot{x}}{\dot{y}}$, and perpendicular to it. Hence we have:

\[\boldsymbol{F}_v = -k \hat{\mathbf{v}} = -k\binom{-\dot{y}}{\dot{x}} = k\binom{\dot{y}}{-\dot{x}}\]

Using Newtons 2nd law:

\[\boldsymbol{F}_{res} = m\binom{\ddot{x}}{\ddot{y}} = \boldsymbol{F}_g + \boldsymbol{F}_v = m\binom{0}{g} +k\binom{\dot{y}}{-\dot{x}}\]

In component form:

\[m\ddot{x} = k\dot{y}\\\\ m\ddot{y} = mg - k \dot{x}\]
Isn't the vector: (\(\displaystyle -k\dot y,k\dot x\)),also perpenticular to the particle velocity and proportional to it ??
 
  • #9
Please post anything relating to the solution of a problem (in the Challenges forum) in [sp]...[/sp] tags. Thanks. :)
 
  • #10
solakis said:
Isn't the vector: (\(\displaystyle -k\dot y,k\dot x\)),also perpenticular to the particle velocity and proportional to it ??

Yes, this vector also fulfills the condition, and you can elaborate on the equations of motion with opposite signs for the velocity dependent force. You´ll see, that the y-component turns out to be the same as before. Only the x-component changes sign, i.e. the direction of motion would be from right to left starting in origo.
 
  • #11
lfdahl said:
Yes, this vector also fulfills the condition, and you can elaborate on the equations of motion with opposite signs for the velocity dependent force. You´ll see, that the y-component turns out to be the same as before. Only the x-component changes sign, i.e. the direction of motion would be from right to left starting in origo.

Thanks
I have done this allready
 

FAQ: Particle Motion in a Vertical Plane: Trajectory Equation & Curve

1. What is particle motion in a vertical plane?

Particle motion in a vertical plane refers to the movement of an object or particle in a straight line or curved path in a vertical direction, typically under the influence of gravity.

2. What is the trajectory equation for particle motion in a vertical plane?

The trajectory equation for particle motion in a vertical plane is y = -gt^2 + v0t + y0, where y is the vertical position, t is time, g is the acceleration due to gravity, v0 is the initial velocity, and y0 is the initial vertical position.

3. How is the trajectory equation derived?

The trajectory equation is derived from the equations of motion, specifically the vertical position equation y = y0 + v0t + 1/2at^2, where y0 is the initial vertical position, v0 is the initial velocity, and a is acceleration. By setting a = -g (acceleration due to gravity) and rearranging the equation, we get the trajectory equation for particle motion in a vertical plane.

4. How does the trajectory equation account for curved paths?

The trajectory equation accounts for curved paths by allowing for the initial velocity v0 to have both horizontal and vertical components. These components can be manipulated to change the direction of the particle's motion, resulting in a curved path.

5. What are some real-world applications of particle motion in a vertical plane?

Particle motion in a vertical plane is used in a variety of real-world applications, such as analyzing the trajectory of projectiles in sports like baseball or golf, predicting the flight path of a rocket or missile, and understanding the motion of objects in free fall. It is also essential in engineering and physics for designing and testing structures and machines that involve vertical motion.

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