Physics, asked by krishch3579, 4 months ago

The range of two projectiles launched from ground

with the same initial velocity u and angles of

projection 1 and 2 are equal. The ratio of

maximum heights reached by them is h

h

1

2

1

3

 . The

range of projectiles R is equal to

(1) u

g

2

2

(2) u

g

2

3

2

(3)

2

4

u

g

(4) u

g

2​

Answers

Answered by shyamkumarsingh06
0

Answer:

3, u is correct answer but g is correct

Answered by nirman95
25

Correct Question:

the range of two projectiles launched from ground with the same initial velocity u and angles of projection theta 1 and theta 2 are equal .the ratio of maximum heights reaches by them is h1/h2 =1/3. The range of projectiles R is equal to?

a. u²/2g

b. 2u²/ g

c. u² /4g

d. √3u²/2g

Calculation:

Always remember that :

  • Two projectiles when thrown at complementary angle of projections with the same speed have same value of range.

  • So, if one angle of projection is θ , then the other angle of projection will be (90°- θ).

Since h1 : h2 = 1 : 3 , let the heights be x and 3x.

For 1st Projectile:

\therefore \: h1 = \dfrac{ {u}^{2} { \sin}^{2}( \theta) }{2g}

\implies\: x= \dfrac{ {u}^{2} { \sin}^{2}( \theta) }{2g}

For 2nd Projectile:

\therefore \: h2= \dfrac{ {u}^{2} { \sin}^{2}( {90}^{ \circ} - \theta) }{2g}

\implies \: h2= \dfrac{ {u}^{2} { \cos}^{2}( \theta) }{2g}

\implies \:3x= \dfrac{ {u}^{2} { \cos}^{2}( \theta) }{2g}

Dividing the equations:

\therefore \: \dfrac{ { \sin}^{2}( \theta) }{ { \cos}^{2} ( \theta)} = 3

\implies \: { \tan}^{2} ( \theta) = 3

\implies \: \tan( \theta) = \sqrt{3}

\implies \: \theta= {60}^{ \circ}

Now , let range be R:

\therefore \: R = \dfrac{ {u}^{2} \sin(2 \theta) }{g}

\implies \: R = \dfrac{ {u}^{2} \sin(2 \times {60}^{ \circ} ) }{g}

\implies \: R = \dfrac{ {u}^{2} \sin( {120}^{ \circ} ) }{g}

\implies \: R = \dfrac{ {u}^{2} \sin( {180}^{ \circ} - {60}^{ \circ} ) }{g}

\implies \: R = \dfrac{ {u}^{2} \sin( {60}^{ \circ} ) }{g}

\implies \: R = \dfrac{ {u}^{2} \times \frac{ \sqrt{3} }{2} }{g}

\implies \: R = \dfrac{ \sqrt{3} {u}^{2} }{2g}

So, final answer is:

\boxed{ \bold{ \: R = \dfrac{ \sqrt{3} {u}^{2} }{2g} }}

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