Slope and Projectile Problem: Finding Distance Covered on a Landing Slope

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Homework Help Overview

The problem involves a ski-jump scenario where Eddie "The Eagle" Edwards takes off with a horizontal velocity and is to determine the distance covered along a slope. The context includes elements of projectile motion and the geometry of the slope.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the meaning of the given distance of 90 m and its relevance to the problem, with some suggesting it may not be necessary for solving the question. Others explore the relationship between horizontal velocity and the slope's gradient, questioning the applicability of conservation of energy and projectile motion equations.

Discussion Status

The discussion is ongoing with various interpretations being explored. Some participants have suggested focusing on the equations of motion and the intersection of the skier's trajectory with the slope, while others express confusion about the mathematical representation of the problem.

Contextual Notes

Participants note the lack of explicit information regarding the slope's angle and the implications of the given data. There is also mention of the need to convert parametric equations to Cartesian form for analysis.

  • #31
gneill said:
Nope. Accelerated motion. What's the equation of motion for an object undergoing acceleration? It should be in your notes or text.

There are two
one is

v2 - v1 / t = a

and the other

v2^2 - v1^2 / 2d = a
 
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  • #32
Lolagoeslala said:
There are two
one is

v2 - v1 / t = a

and the other

v2^2 - v1^2 / 2d = a

Okay, those are fine if you happen to know the initial and final velocities, v1 and v2. But here you're interested in distance with respect to time; the only variables should be distance and time. y = ...

So, what equation of (accelerated) motion fits the bill?
 
  • #33
gneill said:
Okay, those are fine if you happen to know the initial and final velocities, v1 and v2. But here you're interested in distance with respect to time; the only variables should be distance and time. y = ...

So, what equation of (accelerated) motion fits the bill?

ok in that case it would be
2d/t^2 = a
 
  • #34
Lolagoeslala said:
ok in that case it would be
2d/t^2 = a

That'll do. Now make the distance variable y. Write it in the form y = ...

What symbol should you use in place of a for gravitational acceleration?
 
  • #35
gneill said:
That'll do. Now make the distance variable y. Write it in the form y = ...

What symbol should you use in place of a for gravitational acceleration?

y = gt^2/2
 
  • #36
Lolagoeslala said:
y = gt^2/2

Okay. Now, is y increasing or decreasing in value as time moves forward? (Is the skier rising or falling?)
 
  • #37
gneill said:
Okay. Now, is y increasing or decreasing in value as time moves forward? (Is the skier rising or falling?)

he is falling so there needs to be a negative sign infront of it
 
  • #38
Lolagoeslala said:
he is falling so there needs to be a negative sign infront of it

Good.

Now, you've got your two parametric equations for the trajectory:

##x(t) = v_x t##

##y(t) = -\frac{1}{2}g t^2##

Can you combine them to write y in terms of x? (that is, eliminate t in the equation for y)
 
  • #39
gneill said:
Good.

Now, you've got your two parametric equations for the trajectory:

##x(t) = v_x t##

##y(t) = -\frac{1}{2}g t^2##

Can you combine them to write y in terms of x? (that is, eliminate t in the equation for y)

y(t) = - 1/2 g (x/v)^2
 
  • #40
Lolagoeslala said:
y(t) = - 1/2 g (x/v)^2

Alright. But no y(t) any more. It's y(x). The t has been eliminated. That's the equation of the parabola that the skier follows.

So now you have the equation of the line representing the ski slope and the parabola representing the skier's path. Can you find their intersection?
 
  • #41
gneill said:
Alright. But no y(t) any more. It's y(x). The t has been eliminated. That's the equation of the parabola that the skier follows.

So now you have the equation of the line representing the ski slope and the parabola representing the skier's path. Can you find their intersection?

y(x) = - 1/2 g (x/v)^2
x = -3/4

y(x) = - 1/2 g (-3/4v)^2
y(x) = - 1/2 g (-3/4v)^2
y(x) = 0.00689
 
  • #42
Lolagoeslala said:
y(x) = - 1/2 g (x/v)^2
x = -3/4 <---
No, that's not right; x is not a constant. Where's your equation for the line? Look back to posts #23 and #24.
 
  • #43
y =- 3/4x
y(x) = - 1/2 g (x/v)^2


-3/4x = -1/2g(x/v)^2
3/4x = 1/2g(x/v)^2
3/4x = 1/2gx^2/v^2
2 x 3/4 x v^2 / g= x
600/g = x
61.22 = x
 
  • #44
Lolagoeslala said:
y =- 3/4x
y(x) = - 1/2 g (x/v)^2


-3/4x = -1/2g(x/v)^2
3/4x = 1/2g(x/v)^2
3/4x = 1/2gx^2/v^2
2 x 3/4 x v^2 / g= x
600/g = x
61.22 = x

That looks better!

So that's the value of x where the curves intersect. Can you now find L, the distance along the slope?
 
  • #45
gneill said:
That looks better!

So that's the value of x where the curves intersect. Can you now find L, the distance along the slope?

ok so i know where they intersect which is 61.22
wouldn't the length be 61.22 too?
 
  • #46
Lolagoeslala said:
ok so i know where they intersect which is 61.22
wouldn't the length be 61.22 too?

Nope. That's the horizontal distance. You're looking for the distance along the slope. The 'L' in your diagram.
 
  • #47
Ok i see so itll be like this..

horizontal distance = 61.22 m
L = ?
Angle = 37°

cos 37° = a/61.22 m
cos 37°x 61.22m = a
and the L is 48.89 m
 
  • #48
Lolagoeslala said:
Ok i see so itll be like this..

horizontal distance = 61.22 m
L = ?
Angle = 37°

cos 37° = a/61.22 m
cos 37°x 61.22m = a
and the L is 48.89 m

Bit of a problem with your working there. Consider,... is the hypotenuse of a triangle ever shorter than either of the other sides? Here L is the hypotenuse of a triangle with one side of length 61.22 m. Draw your triangle with the 'x' side and 'L' hypotenuse in place and redo the calculation.
 
  • #49
gneill said:
Bit of a problem with your working there. Consider,... is the hypotenuse of a triangle ever shorter than either of the other sides? Here L is the hypotenuse of a triangle with one side of length 61.22 m. Draw your triangle with the 'x' side and 'L' hypotenuse in place and redo the calculation.

http://s1176.beta.photobucket.com/user/LolaGoesLala/media/Untitled_zps4a736718.jpg.html#/user/LolaGoesLala/media/Untitled_zps4a736718.jpg.html?&_suid=135745223970705186732013962768

like this?
 
  • #50
Lolagoeslala said:
http://s1176.beta.photobucket.com/user/LolaGoesLala/media/Untitled_zps4a736718.jpg.html#/user/LolaGoesLala/media/Untitled_zps4a736718.jpg.html?&_suid=135745223970705186732013962768

like this?

Yup. Be sure to indicate where the known angle is.

Alternatively, you could use geometry and similar triangles since you know that this triangle is similar to the 3-4-5 triangle from your initial diagram.
 
  • #51
Okay so what i was thinking was i could find the side that is opposite to the angle
so like

tan 37 = o / 61.22 m
o = 46.13 m

and use a^2 = b^2 + c^2
a^2 = (61.22m)^2 + (46.13m)^2
a= 76.6 or 77
 
  • #52
Lolagoeslala said:
Okay so what i was thinking was i could find the side that is opposite to the angle
so like

tan 37 = o / 61.22 m
o = 46.13 m

and use a^2 = b^2 + c^2
a^2 = (61.22m)^2 + (46.13m)^2
a= 76.6 or 77

That'll do it. But it's kind of taking the long way around :smile:

You can write ##cos(\theta) = x/L## so that ##L = x/cos(\theta)##, and cos(θ) can be obtained from the similar 3-4-5 triangle as cos(θ) = 4/5.

attachment.php?attachmentid=54489&stc=1&d=1357477300.gif


Or, avoiding trig functions altogether, you can use the "raw geometry" of similar triangles:

##\frac{L}{x} = \frac{5}{4}## so that ##L = x \frac{5}{4}##

where x is 61.18 m, of course.
 

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  • #53
THANK YOU SO MUCH FOR YOUR HELP!
u r like a god to me :D
 
  • #54
Lolagoeslala said:
THANK YOU SO MUCH FOR YOUR HELP!
u r like a god to me :D

Careful, my ego may explode :eek:

Glad I could help. Cheers!
 

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