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Question 14
The take-off point O on a ski jump is located at the top of a downslope. The angle between the downslope and the horizontal is $rac{ heta}{4}$. A skier takes off ... show full transcript
Step 1
Answer
To derive the required equation, we begin with the expressions given for the flight path:
From the equations of motion, we have:
y = rac{1}{2} g t^2 + V ext{sin} heta imes t
Here, is the time in seconds after take-off.
Rearranging the first equation for , we get:
t = rac{x}{V ext{cos} heta}.
Substituting this expression for into the second equation:
y = rac{1}{2} g igg( rac{x}{V ext{cos} heta} igg)^2 + V ext{sin} heta igg( rac{x}{V ext{cos} heta} igg).
Simplifying this gives:
y = rac{g x^2}{2V^2 ext{cos}^2 heta} + x an heta.
Finally, rearranging leads us to the expression:
y = x an heta - rac{g x^2}{2V^2 ext{sec}^2 heta}.
Step 2
Answer
To derive the expression for D, we will utilize the results from part (i).
Recognizing the equation for the flight path, we find where the skier lands on the slope given by:
D = x_{max} = rac{V^2 ext{sin}(2 heta)}{g}.
The maximum distance D in terms of θ is obtained when is maximized, which occurs when , or .
Thus, substituting gives:
D = 2 rac{V^2}{g}.
Step 3
Answer
To find the derivative of D with respect to θ, begin from the expression of D derived previously:
Differentiating D with respect to θ using the chain rule:
rac{dD}{d heta} = rac{d}{d heta}igg(rac{V^2 ext{sin}(2 heta)}{g}igg).
Applying the derivative gives:
rac{dD}{d heta} = rac{2V^2 ext{cos}(2 heta)}{g}.
Recognizing that can be related as well leads to:
rac{dD}{d heta} = 2 rac{ ext{V}^2}{g ext{sin}(2 heta)}.
Step 4
Answer
To find the maximum value of D, we set rac{dD}{d heta} = 0:
From part (iii), set:
2 rac{V^2}{g ext{sin}(2 heta)} = 0.
This indicates that , giving:
2 heta = nrac{ ext{π}}{2}, ext{ } n ext{ integer}.
The maximum occurs at:
.
However, as we seek a valid angle in the context of the problem, the value of θ for maximum distance occurs at 45°, resulting in peak D.
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