Maximum perpendicular height above an inclined plane

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Homework Help Overview

The problem involves a particle projected from a point on an inclined plane at an angle of 60° to the horizontal, with the projection angle denoted as ∅. The goal is to prove a relationship for the maximum perpendicular height, H, in terms of the initial velocity, u, and gravitational acceleration, g.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the decomposition of the initial velocity into components along the inclined plane and question the validity of the angle used in the calculations. Some express concern about the implications of the angle ∅ in relation to the incline and the conditions under which the height H is defined.

Discussion Status

The discussion is ongoing, with various interpretations of the problem being explored. Some participants suggest that the original formulation may not account for the correct angle of projection relative to the incline, while others offer alternative expressions for the maximum height based on different assumptions.

Contextual Notes

There is uncertainty regarding the conditions under which the angle ∅ is defined, particularly whether it should be greater than 60°. Participants also note the potential for confusion regarding the definition of "perpendicular height" in relation to the inclined plane.

Woolyabyss
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Homework Statement


A particle is projected from a point o with initial velocity u up a plane inclined at an angle 60° to the horizontal. The direction of projection makes an angle ∅ with the horizontal. The maximum perpendicular height is H.

prove that H = u^2( sin^2(∅) ) / g

Homework Equations



v = u + at

s = ut + .5(a)(t^2)


The Attempt at a Solution



the horizontal axis ( i axis ) is the line of greatest slope of the inclined plane. The j axis is perpendicular to the i axis.

splitting the u vector into horizontal and vertical components along the i and j axis'.

i axis..... ucos( ∅ - 60 )

j axis.....usin( ∅ - 60)

force of gravity split into component vectors along and perpendicular to the inclined plane

i axis = gsin(60) = √3/2

j axis = (1/2)g


the object will have reached its maximum perpendicular height when its vertical velocity(Vy) is 0

Vy = usin(∅ - 60) - (1/2)gt = 0

t = 2u( sin( ∅ - 60 ) )/g

The maximum perpendicular height Sy = H

Sy = ut + (1/2)at^2

Sy = usin(∅-60)(2u)(sin(∅-60)/g -(1/2)(1/2)g(4u^2)( sin^2(∅-60)/g^2 )

simplify

Sy = u^2( sin^2( ∅ - 60 ) ) /g

when I simplify using

sin(A-B)=sin A cos B - cos A sin B

It just makes the equation more awkward

I think I was right using ∅ - 60 since both angles are taken from the horizontal so you have to subtract to get the angle between the objects line of projection and the plane.

Any help would be appreciated.
 
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Woolyabyss said:

Homework Statement


A particle is projected from a point o with initial velocity u up a plane inclined at an angle 60° to the horizontal. The direction of projection makes an angle ∅ with the horizontal. The maximum perpendicular height is H.

prove that H = u^2( sin^2(∅) ) / g

I worry that there is an H value that results if ∅ = 30o, but it is not possible to project the particle up a 60o incline if you project it at 30o to the horizontal ?

Perhaps the condition ∅ > 60o is implied.

The expression H = u^2( sin^2(∅) ) / g is merely the maximum height reached by any projectile fired at an angle ∅ with the horizontal.
 
Can someone explain the problem here?
 
PeterO said:
I worry that there is an H value that results if ∅ = 30o, but it is not possible to project the particle up a 60o incline if you project it at 30o to the horizontal ?
That doesn't bother me. The equation merely gives a parabolic trajectory which includes the point of origin of the particle. The slope must either be a tangent to the trajectory or cut it in two places, with a finite section of the trajectory above the slope.
The given result is clearly wrong, though. If the particle is fired parallel to the slope then H must be 0. Woolyabyss' answer, u2 sin2(∅-60)/g, is much more reasonable. Maybe the question should have said it makes an angle ∅ with the plane.
 
I'm not sure then, I think I'll just leave this question and move on.
 
Last edited:
You can throw that particle from the slope at an angle θ>60° to the horizontal. The maximum height it reaches depends on the vertical component of its velocity , independent of the slope. H=(usinθ)2/2g.

ehild
 
ehild said:
You can throw that particle from the slope at an angle θ>60° to the horizontal. The maximum height it reaches depends on the vertical component of its velocity , independent of the slope. H=(usinθ)2/2g.

ehild

Yes, but it's asking for the "perpendicular height", which Woolyabyss and I interpret as the max distance from the plane.
 
Maybe it should have written that θ is the angle with respect to the slope. Choosing y perpendicular to the slope, y=usin(θ)t-gcos(60) t2/2. As cos60=1/2, y=usin(θ)t-g t2/4. Its maximum is H=u2sin2(θ)/g, the given solution.

ehild
 

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