Projectile Motion, leaping the river

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Homework Help Overview

The discussion revolves around a projectile motion problem involving a rider attempting to leap across a river from an inclined ramp. The ramp's angle, the width of the river, and the height difference between the ramp and the far bank are specified. Participants are exploring methods to determine the initial velocity required for the rider to successfully reach the opposite bank.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants are examining the application of projectile motion equations, questioning the appropriateness of methods used given the height difference involved. Some express confusion about the initial and final height definitions in the context of the problem.

Discussion Status

There is an ongoing exploration of the problem, with participants offering different perspectives on the equations used and the assumptions made regarding height and displacement. Some participants have noted potential errors in the original poster's approach, while others are clarifying the implications of height on the projectile's trajectory.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can use or the methods they can apply. The discussion includes varying interpretations of the problem setup, particularly regarding the initial and final heights in the projectile motion equations.

rocomath
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i'm curious to know whether my method is the long way or perhaps, the only way in solving for initial velocity for this problem

if you have a faster way, i'd like to see it ... I'm trying to be efficient!

The take off ramp is inclined at 53.0, the river is 40.0m wide, and the far bank is 15.0m lower than the top of the ramp. The river itself is 100m below the ramp. (Ignore air resistance) a) What should his speed have been at the top of the ramp to have just made it to the edge of the far bank?

http://i110.photobucket.com/albums/n104/rox1co/leapingtheriver2.jpg

http://www.mathlinks.ro/Forum/latexrender/pictures/e/b/2/eb21343a1e34a55256a7b86eed1fdf89c8f1b0f8.gif
 
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In this problem y and g are in the down ward direction and initial velocity is in the upward direction. Therefore y and g must have the same sign and velocity should be opposite sign.
There is no shortcut method to solve this problem.
 
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I think that there is something wrong.

The equations which you have applied is for a projectile motion on a horizontal plane.

But here the rider is starting from a height of 15 m.

And by the equations which you have applied it means that if the bike launches at a speed of 17.8 m/s he would be at the other end of the bank but at the height of 15m and hence its range would be greater than 40m.
 
FedEx said:
I think that there is something wrong.

The equations which you have applied is for a projectile motion on a horizontal plane.

But here the rider is starting from a height of 15 m.

And by the equations which you have applied it means that if the bike launches at a speed of 17.8 m/s he would be at the other end of the bank but at the height of 15m and hence its range would be greater than 40m.
it's correct since it's also the answer at the back of the book. i took [tex]y_{0}[/tex] to be 0 which is at the point as he leaves the ramp and [tex]y=-15m[/tex] unless i lucked out.
 
rocophysics said:
it's correct since it's also the answer at the back of the book. i took [tex]y_{0}[/tex] to be 0 which is at the point as he leaves the ramp and [tex]y=-15m[/tex] unless i lucked out.

OK. It gets solved if you take

[tex]y_0 = 0[/tex]

and

[tex]y = -15[/tex]
 
FedEx said:
OK. It gets solved if you take

[tex]y_0 = 0[/tex]

and

[tex]y = -15[/tex]
first i thought i would have to find the max height reached, and then go from there. i just find it strange that the descent isn't actually -15m, but i guess the rider barely goes above y=0 so it's negligible.

physics is weird to me.
 
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rocophysics said:
first i thought i would have to find the max height reached, and ten go from there. i just find it strange that the descent isn't actually -15m, but i guess the rider barely goes above y=0 so it's negligible.

physics is weird to me.

The point is that it doesn't matter how high above y=0 the rider travels; it is the total displacement that the equation depends upon. If he has a maximum height of 20m, say, he will have to come back down from 20m high, and so the net displacement of this motion will be zero.
 
cristo said:
The point is that it doesn't matter how high above y=0 the rider travels; it is the total displacement that the equation depends upon. If he has a maximum height of 20m, say, he will have to come back down from 20m high, and so the net displacement of this motion will be zero.


But the projectile is committed at a height of 15 m. Hence if we consider the initial height as 0 then we have to consider the final height as -15 m.
 
FedEx said:
But the projectile is committed at a height of 15 m. Hence if we consider the initial height as 0 then we have to consider the final height as -15 m.

Perhaps I didn't explain it well enough, but I was merely trying to point out why any distance the rider goes vertically over the line y=0 did not add on to the total displacement.
 
  • #10
leaping the river

I am working on this problem and have can't seem to find a solution. The answer needs to be in variable form and my answer doesn't seem accurate. Any help would be great.


Leaping the River. A car of weight W_C car comes to a bridge during a storm and finds the bridge washed out. The driver of weight W_D must get to the other side, so he decides to try leaping it with his car. The side the car is on is h_1 above the river, while the opposite side is a mere h_2 above the river. The river is L wide.
 
  • #11
How fast should the car be traveling just as it leaves the cliff in order just to clear the river and land safely on the opposite side?

What is the speed of the car just before it lands safely on the other side?
 

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