Physics, asked by shipra2509, 1 year ago

please give me the solution it is urgent please please please​

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Answered by devanayan2005
5

a body is projected at an angle 60° with horizontal.

given, horizontal range = 6m + 3m = 9m

let initial speed of body is u

then, horizontal range = u²sin2(60°)/g

or, 9m = u² sin120°/10

or, 90 = u² × sin(180 - 60°)

or, 90 = u² sin60°

or, 90 = u² × √3/2

or, u² = 60√3 ......(1)

now, applying formula,  along horizontal direction.

here, x = 6m,  and ax = 0

so, 6 = ucos60° t

or, t = 6/ucos60° = 12/u.......(2)

applying formula,

here, uy = usin60° , t = 12/u [ from equation (2) ] and ay = -g

then, y = usin60° × 12/u - 1/2 × g × 144/u²

= 12sin60° - g × 72/u²

putting g = 10m/s² and u² = 60√3 from equation (1),

y = 12 × √3/2 - 10 × 72/60√3

= 6√3 - 12/√3

= 6√3 - 4√3

= 2√3

hope helps

Answered by QGP
26

Trajectory Equation - Projectile Motion

Question:

A body is projected at an angle of 60^{\circ} with horizontal. Its Range is 9 m. When x = 6 m, the value of y for the projectile would be:

Answer:

We have the data:

\sf \theta = 60^{\circ} \\\\ \sf R = 9\ m\\\\ y =\ ?\ at\ x = 6\ m

We will use the Trajectory Equation to directly relate x and y, but first we must find the initial velocity \sf u. And we will do this by using the formula of Range.

\sf\displaystyle R = \frac{u^2\, sin\, 2\theta}{g}\\\\\\\sf \implies u^2 = \frac{gR}{2\, sin\, \theta \, cos\, \theta} \\\\\\\sf \implies u^2 = \frac{10\times 9}{2\times sin\, 60^{\circ}\times cos\, 60^{\circ}} \\\\\\\sf \implies u^2 = \frac{10\times 9}{2\times\frac{\sqrt{3}}{2}\times \frac{1}{2}} \\\\\\\sf \implies u^2 = \frac{180}{\sqrt{3}}

Now, we can use the Trajectory Equation and substitute \sf u^2

\sf\displaystyle y = x\, tan\, \theta - \frac{gx^2}{2u^2\, cos^2\, \theta}\\\\\\\sf\implies y=6\, tan\, 60^{\circ}-\frac{10\times 6^2}{2\times \frac{180}{\sqrt{3}}\times cos^2\, 60^{\circ}}\\\\\\\sf \implies y=6\sqrt{3}-\frac{10\times 36\times \sqrt{3}}{2\times 180\times \frac{1}{4}} \\\\\\ \sf\implies y=6\sqrt{3}-4\sqrt{3}\\\\\\\sf\implies {\Large\boxed{\sf y=2\sqrt{3}\ m}} \ \textsf{Option (2)}

Thus, The Answer is Option (2): \sf 2\sqrt{3}\ m.

 \rule{320}{1}

Alternative Method:

This is a slightly different method. Here, we will directly modify the trajectory equation to use the parameters we already know.

Consider the Trajectory Equation:

\sf\displaystyle y=x\, tan\, \theta-\frac{gx^2}{2u^2\, cos^2\,\theta}\\\\\\ \textsf{Let's modify the second term to bring R}\\\\\\ \sf\implies y = x\, tan\, \theta-\frac{gx^2}{2u^2\, cos^2\,\theta}\times\frac{sin\,\theta}{sin\,\theta}\\\\\\\sf\implies y = x\, tan\, \theta-\frac{g}{2u^2\, sin\,\theta\, cos\,\theta}\times\frac{x^2\ sin\,\theta}{cos\,\theta}\\\\\\\sf\implies y = x\, tan\, \theta-\frac{ x^2\, tan\,\theta}{R}\\\\\\ \implies \boxed{\sf y=x\, tan\,\theta\left(1-\frac{x}{R}\right)}

This is another form of the trajectory equation, which uses Range instead of the initial velocity.

We can use this another form directly for our question.

\sf\displaystyle y=x\, tan\,\theta\left(1-\frac{x}{R}\right) \\\\\\ \implies \sf y = 6\, tan\, 60^{\circ}\left(1-\frac{6}{9}\right)\\\\\\ \implies \sf y = 6\sqrt{3}\left(1-\frac{2}{3}\right)\\\\\\ \implies \sf y=6\sqrt{3}\times \frac{1}{3}\\\\\\ \implies {\Large\boxed{\sf y=2\sqrt{3}\ m}}\ \textsf{Option (2)}

This method made our calculations a lot simpler. Anyway, The Answer is Option (2).

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