A gun has a muzzle speed of 80 meters per second. What angle of elevation should be used to hit an object 180 meters away? Neglect air resistance and use g=9.8m/sec2 as the acceleration of gravity. The answer must be in radians. I found: angle=1/2arcsin (180*9.8)/(80^2), but it was not correct.
The way to tackle this problem is to understand it as components of Vertical and Horizontal velocities. First, The vertical distance can be defined in terms of it's verticle velocity & the acceleration applied, as shown below: \[s = s_o + v_o \times t + (a \times t^2 / 2)\] Initial vertical distance, \[s_o = 0m.\] Final vertical distance, \[s = 0m.\] The assumption is that the object has the same elevation as the the spot where the gun is being fired. Initial vertical velocity is \[v_v = 80 \times \sin \theta\], so the above equation becomes \[0 = 80 \times \sin \theta \times t + 4.9 \times t^2 ...... (1)\] The distance horizontally to be covered is 180m. Since the assumption of no drag being applied then there is no deceleration in this case, this gives \[v_h = 80 \cos \theta\] Substitute this into the top equation we get: \[180 = 80 \cos \theta \times t\] Rearrange and we get: \[t = 180 / (80 \cos \theta) ............ (2)\] Substitute (2) into (1) you get \[(24.8 / \cos^2 \theta) + (180 \sin \theta / \cos \theta) = 0\] Multiply the right term by \[\cos \theta / \cos \theta\] and rearrange you get \[\sin \theta \cos \theta = -24.8/180\ ........(3)\] Now \[\sin (2\theta) = 2 \sin \theta \cos \theta\] so equation (3) becomes \[\sin(2 \theta) = -49.6/180\] Solve and you get\[\theta = -0.1396 radians\] i.e. the gun is firing to the left at 8 degrees from the horizon.
I need to correct what I wrote. Some of the signs are incorrect in the working out. It should be 0.1396radians if you are going from left to right. I'm not sure what I did wrong. I'm sure you can work it out.
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