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Question: A particle aimed at a target, projected with an angle \({15^ \circ }\) with the horizontal is short ...

A particle aimed at a target, projected with an angle 15{15^ \circ } with the horizontal is short of the target by 10m10m. If projected with an angle of 45{45^ \circ } is away from the target by 15m15m, then the angle of projection to hit the target is:
A) 12sin1(110)\dfrac{1}{2}{\sin ^{ - 1}}\left( {\dfrac{1}{{10}}} \right)
B) 12sin1(310)\dfrac{1}{2}{\sin ^{ - 1}}\left( {\dfrac{3}{{10}}} \right)
C) 12sin1(910)\dfrac{1}{2}{\sin ^{ - 1}}\left( {\dfrac{9}{{10}}} \right)
D) 12sin1(710)\dfrac{1}{2}{\sin ^{ - 1}}\left( {\dfrac{7}{{10}}} \right)

Explanation

Solution

Here we will be using a concept of projectile motion. And applying a range of projectile formulas to calculate angle of projectile. Anybody projected into the air at an angle other than 90{90^ \circ } with the horizontal is called projectile motion. There are three parameters which are related to projectile motion.

Formula used: Range of projectile,
R=u2sin2θgR = \dfrac{{{u^2}\sin 2\theta }}{g}
Where, uu is velocity of projection, θ\theta is angle of projection, gg is acceleration due to gravity, g=9.8ms2g = 9.8m{s^{ - 2}}

Complete step-by-step answer:
Given, case (i)θ=150\theta = {15^{^0}}
Let ‘xx’ be the horizontal range travelled by the projectile which we need to calculate.
R1=u2sin2θg\Rightarrow {R_1} = \dfrac{{{u^2}\sin 2\theta }}{g}...................... (a)

Here R1{R_1} is the horizontal distance travelled by the projectile at an angle 150{15^{^0}}. Then from figure,
Here, a particle is projected at an angle of 150{15^{^0}} and it has reached 10m10m short before reaching the target.
R1=x10\Rightarrow {R_1} = x - 10
Substitute in equation (a) we get,
x10=u2sin2×15g\Rightarrow x - 10 = \dfrac{{{u^2}\sin 2 \times 15}}{g}
x10=u2sin30g\Rightarrow x - 10 = \dfrac{{{u^2}\sin {{30}^ \circ }}}{g}
Here we can substitute the trigonometry value
sin300=12\Rightarrow \sin {30^0} = \dfrac{1}{2}
u22g=x10\Rightarrow \dfrac{{{u^2}}}{{2g}} = x - 10 ……………….. (1)
Case (ii) θ=450\theta = {45^{^0}}
Here R2{R_2} is the horizontal distance travelled by the projectile at an angle450{45^{^0}}. Then from figure,
R2=x+15\Rightarrow {R_2} = x + 15
A particle is projected at an angle of 450{45^{^0}} and it has reached a point which is 15m15m away from the target.
R2=u2sin2θg\Rightarrow {R_2} = \dfrac{{{u^2}\sin 2\theta }}{g}
x+15=u2sin2×45g\Rightarrow x + 15 = \dfrac{{{u^2}\sin 2 \times 45}}{g}
We have,
sin900=1\Rightarrow \sin {90^0} = 1
from the trigonometry formula we get
x+15=u2sin900g\Rightarrow x + 15 = \dfrac{{{u^2}\sin {{90}^0}}}{g}
x+15=u2g\Rightarrow x + 15 = \dfrac{{{u^2}}}{g} ………….. (2)
Substitute equation (2) in (1), we get
x+152=x10\Rightarrow \dfrac{{x + 15}}{2} = x - 10
x+15=2x20\Rightarrow x + 15 = 2x - 20
x=35m\Rightarrow x = 35{\text{m}}
x=m\because x = m
After substituting the value of xx in equation (2),
u2g=50\Rightarrow \dfrac{{{u^2}}}{g} = 50
Now we can calculate angle of projectionθ\theta ,
R=u2sin2θg\Rightarrow R = \dfrac{{{u^2}\sin 2\theta }}{g}
35=50×sin2θ\Rightarrow 35 = 50 \times \sin 2\theta
710=sin2θ\Rightarrow \dfrac{7}{{10}} = \sin 2\theta
2θ=sin1(710)\Rightarrow 2\theta = {\sin ^{ - 1}}\left( {\dfrac{7}{{10}}} \right)
θ=12sin1(710)\therefore \theta = \dfrac{1}{2}{\sin ^{ - 1}}\left( {\dfrac{7}{{10}}} \right)

Thus, the correct option is (D).

Note: (i) Time of flight: Total time to reach the horizontal surface of the projectile is called time of flight. It is the total time for which the projectile remains in air.
(ii) Maximum height: The vertical displacement of the projectile during time of ascent (For a projectile the time to reach maximum height).
(iii) Horizontal range: The horizontal distance covered by the projectile during its motion.