A projectile is fired with initial speed v0 = 37.0 m/s from level ground at a target that is on the ground, at distance R = 13.0 m, as shown in the figure. What are the (a) least and (b) greatest launch angles that will allow the projectile to hit the ?

2 Answers
May 13, 2018

The greatest possible angle is #87.327^@#, and the least possible angle is #2.673^@#

Explanation:

Draw a diagram, and resolve the velocity into horizontal and vertical components. For now, let the angle the projectile is fired at be #theta#

enter image source here

Begin by finding the time the projectile is in the air for. Do this by considering the vertical component of velocity:

#s=0# total displacement when it falls is 0.
#u=37sintheta#
#a=-g#
#t=T#

Using #s=ut+1/2at^2#

#0=37Tsintheta-1/2gT^2#
#0=T(37sintheta-1/2gT)#
#T=0# or #T=(37sintheta)/(1/2g)#

#T=(74sintheta)/g#

Now we have the time, consider horizontal velocity.

#s=13#
#u=37costheta#
#a=0#
#t=(74sintheta)/g#

Use this to make an equation to find #theta#

Using #s=ut+1/2at^2#
#13=37costheta*74sintheta/g+0#
#13=2738/gsinthetacostheta#
#sinthetacostheta=(13g)/2738#

I'm unsure how to (or if you can) solve this from here. I instead plotted the graphs of #y=sinxcosx# and, (taking #g=9.81#), #y=(13*9.81)/2738#, and looked at the interception points.

enter image source here

From the graph, this holds if the angle is #2.673^@# or #87.327^@#.
This makes the greatest possible angle #87.327^@#, and the least #2.673^@#

May 25, 2018

Let the launch angle be #=theta#
Time #t# to reach the target can be found from horizontal component of velocity. Neglecting air resistance we get

#R=v_(0x)t#
#=>13=(37costheta)t#
#=>t=13/(37costheta)# ......(1)

Time of flight can also be found with the help of kinematic expression using vertical component of velocity.

#s=ut+1/2at^2#

Noting that gravity acts in a direction opposite to the direction of projection we get

#h=v_(0y)t+1/2(-g)t^2#
#0=(37sintheta)t-1/2g t^2#

Solving for #t# we get

#0=t(37sintheta-1/2g t) #
#=>t=0# and #t=(2xx37sintheta)/(g)#

Ignoring #t=0# as trivial solution as being time of projection, we get

#t=(74sintheta)/g# .......(2)

Equating (1) and (2)

#13/(37costheta)=(74sintheta)/g#
#=>2sinthetacostheta=(13g)/1369#
#=>sin 2theta=(13g)/1368# ........(3)
#=>2theta=sin^-1((13xx9.81)/1369)#
#=>2theta=5.35^@#
#=>theta=2.7^@# ......(4)

We know that for an angle #alpha#,

#sinalpha=sin(180-alpha)#

Using this identity we can write (3) as

#sin (180-2theta)=(13g)/1368#

We get

#180-2theta=5.35^@#
#=>theta=(180-5.35)/2#
#=>theta=87.3^@# .......(5)

(a) #2.7^@#
(b) #87.3^@#

.-.-.-.-.-.-.-.-.-.-

In case you can recall it is perfectly fine to use the formula for horizontal range:

#R=(2v_0^2sinθcosθ)/g #
or
#R=(v_0^2sin2θ)/g #