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Question 6
The points A, B, C and D are placed on a circle of radius r such that AC and BD meet at E. The lines AB and DC are produced to meet at F, and BEFC is a cyclic quadri... show full transcript
Step 1
Answer
To find the size of ( \angle DBF ), we utilize the cyclic properties of the quadrilateral BEFC. In a cyclic quadrilateral, opposite angles are supplementary. Therefore:
[ \angle AEF + \angle DBF = 180^{\circ} ]
We can also find ( \angle AEF ) using the inscribed angle theorem. Since ( \angle AEF ) subtends arc AB, we know:
[ \angle AEF = \frac{1}{2}(\text{measure of arc AB}) ]
This implies:
[ \angle DBF = 180^{\circ} - \angle AEF ]
By finding the measure of arc AB, we can compute( \angle DBF ).
Step 2
Answer
To find the length of AD in terms of r, consider triangle ACD, which is inscribed in the circle. By the properties of the circle:
[ AD = 2r \sin \frac{\angle ACD}{2} ]
Let ( \angle ACD = \theta ). Thus we can express AD as:
[ AD = 2r \sin \frac{\theta}{2} ]
Step 3
Answer
To show that the water returns to ground level at the specified distance, we need to set ( y = 0 ) in the parametric equation for y:
[ 0 = v \sin \theta - \frac{1}{2} gt^2 \implies t^2 = \frac{2v \sin \theta}{g} ]
Substituting into the equation for x:
[ x = v \cos \theta \cdot t = v \cos \theta \cdot \sqrt{\frac{2v \sin \theta}{g}} ]
Squaring both sides gives:
[ x^2 = \frac{2v^2 \sin \theta \cos \theta}{g} ]
Using the double angle identity ( \sin 2\theta = 2 \sin \theta \cos \theta ):
[ x^2 = \frac{v^2 \sin 2\theta}{g} ]
Thus the distance is:\n [ \frac{v^2 \sin 2\theta}{8} ]
Step 4
Answer
Given the distance to the wall is 40 meters, we can use the derived path equation. At ( \theta = 15^{\circ} ), substituting x:
[ 40 = \frac{v^2 \sin(30^{\circ})}{8} \implies 40 = \frac{v^2}{16} ]
Thus:
[ v^2 = 640 \implies v^2 = 80g \text{ (when expressing g in metre terms)} ]
Step 5
Answer
Start with the parametric equations:
[ x = v \cos \theta \cdot t \text{ and } y = v \sin \theta t - \frac{1}{2} gt^2 ]
From the x equation, express t:
[ t = \frac{x}{v \cos \theta} ]
Substitute this into the y equation:
[ y = v \sin \theta \left( \frac{x}{v \cos \theta} \right) - \frac{g}{2} \left(\frac{x}{v \cos \theta}\right)^2 ]
This simplifies to:
[ y = x \tan \theta - \frac{g x^2}{2v^2 \cos^2 \theta} ]
Replacing ( \frac{g}{v^2} ) with ( 1/80 ) provides the desired result.
Step 6
Answer
Using the equation derived above, set ( y = 20 ) (height of the wall) and find the critical point:
[ 20 = x \tan(15^{\circ}) - \frac{x^2 \sec^2(15^{\circ})}{160} ]
Solve the quadratic equation to determine if there exists a solution that corresponds to the height of the wall, confirming that the water just clears it.
Step 7
Answer
Set the resulting quadratic equation from the previous step to determine all angles where the water reaches the front of the wall. Analyzing the condition would require solving for ( \theta ) using quadratic formula or similar methods.
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