Titled reference frame, N2L with position and velocity

In summary: sorry, the equation for y is?' y= tan(\phi)x= (sin(\phi)/cos(\phi))x ' is because when you graphed the equation for x, it looks like a parabola.
  • #1
Oblio
398
0
A ball is thrown with initial speed vo up an inclined plane. The plane is inclined at an angle(fi) above the horizontal, and the ball's initial vecity is at an angle (theta) above the plane. Choose the axes with x measured up the slope, y normal to the slope and z across it. Write down Newton's second law using these axes and find the ball's position as a function of time. Show that the ball lands a distance

R=2vo^2(sin(theta)cos(theta+fi))/gcos^2(fi)

from its launch point. Show that for given vo adn (fi), the maximum possible range up the inclined plane is

Rmax=vo^2/g(1+sin(fi))

[Don't know if I'm spelling fi right, I mean this symbol : [tex]\phi[/tex]



How do I approach this? I think the question is written poorly, they mean that the ball is thrown in the air and it lands ON the plane.
Without knowing the velocity how do I find the parabolic motion the ball will make?
 
Physics news on Phys.org
  • #2
I know that N2L for the ball can't just be ma=-mg (or a= -g) since it's still traveling up...
 
  • #3
Oblio said:
A ball is thrown with initial speed vo up an inclined plane. The plane is inclined at an angle(fi) above the horizontal, and the ball's initial vecity is at an angle (theta) above the plane. Choose the axes with x measured up the slope, y normal to the slope and z across it. Write down Newton's second law using these axes and find the ball's position as a function of time. Show that the ball lands a distance

R=2vo^2(sin(theta)cos(theta+fi))/gcos^2(fi)

from its launch point. Show that for given vo adn (fi), the maximum possible range up the inclined plane is

Rmax=vo^2/g(1+sin(fi))

[Don't know if I'm spelling fi right, I mean this symbol : [tex]\phi[/tex]



How do I approach this? I think the question is written poorly, they mean that the ball is thrown in the air and it lands ON the plane.
Without knowing the velocity how do I find the parabolic motion the ball will make?
?? You know the balls inital velocity! It is v0. Further, since you are also told that the ball is initially thrown at angle [itex]\theta[/itex] above the plane you know that the balls initial x component of velocity is [itex]v_0 cos(\theta)[/itex] and the y component is [itex]v_0 sin(\theta)[/itex]. You should be able to show that the balls position at time t is [itex]x= v_0 cos(\theta) t[/itex] and [itex]y= -g/2 t^2+ v_0 sin(/theta)t[/itex] (taking (0,0) as initial position). You can solve the first equation for t: [itex]t= x/(v_0 cos(\theta)[/itex] and put that into the equation for y: [itex]y= -g/(2v_0 cos(\theta)x^2+ (sin(\theta)/cos(\theta))x[/itex] to get the equation of the parabola. Now it is a question of determing where that parabola intersects the line giving the inclined plane. That is, of course, [itex] y= tan(\phi)x= (sin(\phi)/cos(\phi))x[/itex].
 
  • #4
[tex]\phi[/tex] is spelt 'Phi'
 
  • #5
HallsofIvy said:
[itex]y= -g/2 t^2+ v_0 sin(/theta)t[/itex] (taking (0,0) as initial position). You can solve the first equation for t: [itex]t= x/(v_0 cos(\theta)[/itex] and put that into the equation for y: [itex]y= -g/(2v_0 cos(\theta)x^2+ (sin(\theta)/cos(\theta))x[/itex] to get the equation of the parabola. , [itex] y= tan(\phi)x= (sin(\phi)/cos(\phi))x[/itex].

Can you explain to me how you got [itex]y= -g/2 t^2+ v_0 sin(/theta)t[/itex] ?
 
  • #6
I suppose it's mostly the /2t^2 I'm failing to see...
 
  • #7
What are the forces along the plane... what are the forces perpendicular to the plane...
 
  • #8
i see that gravity is affecting v(y), but why /2t^2?
 
  • #9
Oblio said:
i see that gravity is affecting v(y), but why /2t^2?

that's just for the (1/2)gt^2.

Hint: Rotate your sketch... so that the incline is horizontal... now you can treat it like a regular projectile problem... the only differences are the vertical and horizontal accelerations...
 
  • #10
learningphysics said:
that's just for the (1/2)gt^2.

Where does that come from?
 
  • #11
Oblio said:
Where does that come from?

From the kinematics equation d = v0*t + (1/2)at^2

a = -g.
 
  • #12
When the projectile is in the air... the only force acting on it is gravity... what is the component of gravity along the plane... what is the component of gravity perpendicular to the plane...

so what's the component of acceleration along the plane... what's the component of acceleration perpendicular to the plane...
 
  • #13
HallsofIvy said:
You can solve the first equation for t: [itex]t= x/(v_0 cos(\theta)[/itex] and put that into the equation for y: [itex]y= -g/(2v_0 cos(\theta)x^2+ (sin(\theta)/cos(\theta))x[/itex] to get the equation of the parabola. Now it is a question of determing where that parabola intersects the line giving the inclined plane. That is, of course, [itex] y= tan(\phi)x= (sin(\phi)/cos(\phi))x[/itex].

Sorry, duh. 'Brainfart' there Learningphysics.
I more or less understand the steps, but could you explain the logic behind why you put the equation for x into y?

And why is '[itex] y= tan(\phi)x= (sin(\phi)/cos(\phi))x[/itex] ' where the parabola interesets?
 
  • #14
Oblio said:
Sorry, duh. 'Brainfart' there Learningphysics.
I more or less understand the steps, but could you explain the logic behind why you put the equation for x into y?

And why is '[itex] y= tan(\phi)x= (sin(\phi)/cos(\phi))x[/itex] ' where the parabola interesets?

That's HallofIvy's post, not mine. The thing is Halls is considering x along the horizontal... y along the vertical... I think the question wants you to approach the problem a little differently...

Work the problem taking x to be along the plane... y to be perpendicular to the plane... I think it makes the problem a lot easier...
 
  • #15
That it what i was trying to do...

so don't do it the way halls of ivy said? I am not sure where to go with this now...
 
  • #16
Oblio said:
That it what i was trying to do...

so don't do it the way halls of ivy said? I am not sure where to go with this now...

See my previous post about rotating the axes, so that the incline is horizontal...
 
  • #17
yeah that is what i had done originally.
 
  • #18
Oblio said:
yeah that is what i had done originally.

cool. can you show how far you got?
 
  • #19
not very. Not using HallsofIvy's method I'm not sure how to figure the distance and parabolic motion of the ball.
 
  • #20
Oblio said:
not very. Not using HallsofIvy's method I'm not sure how to figure the distance and parabolic motion of the ball.

Given v0 and that the angle at which the ball is launched above the incline is theta... what is the initial velocity along the incline... what is the initial velocity perpendicular to the incline ?
 
  • #21
ok, so i still separate THAT into its x and y coordinates.

vx = vocos(theta) and vy=vosin(theta)
 
  • #22
Oblio said:
ok, so i still separate THAT into its x and y coordinates.

vx = vocos(theta) and vy=vosin(theta)

exactly... now what is the acceleration in the x direction (along the plane)... what is the acceleration in the y direction (perpendicular to the plane) ?
 
  • #23
ay = -g and ax = 0 i believe.
 
  • #24
Oblio said:
ay = -g and ax = 0 i believe.

remember... we're taking x to be along the plane... y to be perpendicular to the plane...
 
  • #25
Oblio said:
ok, so i still separate THAT into its x and y coordinates.

vx = vocos(theta) and vy=vosin(theta)

Yes. I want you to remember this is vx along the plane... vy perpendicular to the plane...

The angle at which which the ball is launched relative to the horizontal is (theta + fi)... so if we were working with the x as the horizontal and y as the vertical it would be:

vx = vocos(theta + fi) and vy=vosin(theta + fi)

But since we're working with x along the plane... y perpendicular to the plane... it is:

vx = vocos(theta) and vy=vosin(theta)
 
  • #26
ay=-gcos(phi) ?
 
  • #27
Oblio said:
ay=-gcos(phi) ?

exactly. And what is ax ?
 
  • #28
ahhh ax=-gsin(phi)
 
  • #29
will i be setting vy to zero and then solving a free fall?
 
  • #30
Oblio said:
ahhh ax=-gsin(phi)

yes, exactly...

So what is the displacement in the y direction... what is the displacement in the x direction?
 
  • #31
Oblio said:
will i be setting vy to zero and then solving a free fall?

I don't understand... the question asks you to find the range in the x direction I believe...
 
  • #32
using kinematics?
 
  • #33
Oblio said:
using kinematics?

yes... what is the displacement along the x direction and y direction... in terms of time...
 
  • #34
d = v0*t + (1/2)at^2
 
  • #35
Oblio said:
d = v0*t + (1/2)at^2

Yes. Now use the values we've calculated for v0 and a for this problem... for the x- direction... and the y-direction...
 

Similar threads

Foucault Pendulum at the North Pole
Replies
9
Views
2K
What Calculations Determine the Volleyball's Trajectory in Projectile Motion?
Replies
33
Views
4K
Projectile Motion of football receiver
Replies
9
Views
4K
Projectile motion on an inclined plane
Replies
7
Views
3K
Initial velocity given time and angle
Replies
8
Views
1K
How Does Angular Velocity Affect the Ball's Position on a Basketball Hoop?
Replies
15
Views
2K
Ball is thrown at the edge of the roof of a building
Replies
31
Views
3K
Position vectors in different frames of reference
Replies
19
Views
4K
Velocity on a moving reference frame
Replies
2
Views
1K
I Galilean relativity in terms of homogeneity
2
Replies
51
Views
3K

Hot Threads

Recent Insights

Back
Top