A projectile is fired with an initial speed of 300 meters per second at an angle of 45 degrees to the horizontal, neglecting air resistance, find: A: The time of the impact. B: The horizontal distance covered (range) in meters and kilometers at the time of the impact. C: The maximum height in meters of the projectile.
Start by finding the x and y components of the velocity vector.|dw:1404611339256:dw|
how do i do that?
Use trigonometry, you need these: \(\sf sin\theta=\dfrac{opposite}{hypotenuse}\) \(\sf cos\theta=\dfrac{adjacent}{hypotenuse}\)
ok so theta is equal to 45 degrees, correct?
yes
should my calculator be in radian or degree mode
if you're using degrees (e.g. \(45^o\)) then it should be in degrees
ok, i though so, i just wanted to check though
both cos theta and sin theta were 212.1320344
sounds good. Now we need to use some kinematic equations, do you know them?
these: \(\sf v_f=v_i+a\Delta t\) \(\sf x_f=x_i+v_o\Delta t +\dfrac{1}{2}a_x(\Delta t)^2\) \(\sf v_f^2=v_i^2+2a_x\Delta x\)
wow, um what do i do with those equations
we need to use one (or several) to find what they asked you for, for example: A: The time of the impact. The motion is that of a projectile we know that it's an inverted parabola, so the initial and final position (when it touches the ground) are the same. \(\sf y_i=y_f=0\) |dw:1404612444052:dw| so we'd use the second equation: \(\sf y_f=y_i+v_o\Delta t +\dfrac{1}{2}a_y(\Delta t)^2\) we also know that the only acceleration is due to gravity, a=-9.8 m/\(s^2\), pluggin stuff in gives: \(\sf 0=0+(212~m/s)\Delta t +\dfrac{1}{2}(-9.8~m/s^2)(\Delta t)^2\) now we just need to solve for \(\sf \Delta t\).
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