A projectile is shot from the ground at an angle of #pi/4 # and a speed of #3 m/s#. Factoring in both horizontal and vertical movement, what will the projectile's distance from the starting point be when it reaches its maximum height?
The distance is
We apply the equation of motion
to calculate the time to reach the greatest height
To find the distance, we apply the equation of motion
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To find the distance from the starting point when the projectile reaches its maximum height, we first need to determine the time it takes to reach the maximum height. This occurs when the vertical component of the projectile's velocity becomes zero. The time to reach maximum height can be found using the formula:
[ t = \frac{v_{y0}}{g} ]
Where: ( v_{y0} ) = initial vertical velocity ( g ) = acceleration due to gravity (approximately ( 9.8 , \text{m/s}^2 ))
Given that the projectile is launched at an angle of ( \frac{\pi}{4} ) radians with a speed of ( 3 , \text{m/s} ), the initial vertical velocity (( v_{y0} )) can be calculated using trigonometric functions:
[ v_{y0} = v_0 \sin(\theta) ]
Substitute the values:
[ v_{y0} = 3 , \text{m/s} \times \sin\left(\frac{\pi}{4}\right) = 3 , \text{m/s} \times \frac{\sqrt{2}}{2} = \frac{3\sqrt{2}}{2} , \text{m/s} ]
[ t = \frac{\frac{3\sqrt{2}}{2}}{9.8} \approx 0.306 , \text{s} ]
Now, to find the horizontal distance traveled at the maximum height, we use the time calculated:
[ d_{x\text{ max}} = v_{x0} \times t ]
Where: ( v_{x0} ) = initial horizontal velocity
Given that ( v_{x0} = v_0 \cos(\theta) ):
[ v_{x0} = 3 , \text{m/s} \times \cos\left(\frac{\pi}{4}\right) = 3 , \text{m/s} \times \frac{\sqrt{2}}{2} = \frac{3\sqrt{2}}{2} , \text{m/s} ]
[ d_{x\text{ max}} = \frac{3\sqrt{2}}{2} , \text{m/s} \times 0.306 , \text{s} \approx 0.459 , \text{m} ]
So, the projectile's distance from the starting point when it reaches its maximum height is approximately ( 0.459 , \text{m} ).
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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