Physics, asked by swethavenu2002, 9 months ago

pls give me the step by step ans for this question guys​

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Answered by shadowsabers03
12

Let a coordinate system be introduced in the system where,

  • O is taken as the origin.

  • x axis should be along PQ such that +x is from O to Q, and -x is from O to P.

  • y axis should be along RO such that +y is from O to R.

Given that the mass of each particle is 1 kg.

So the gravitational force of attraction experienced by the mass placed at R due that at P is,

\displaystyle\longrightarrow F_P=\dfrac{G}{2L^2}\ \sf{along\ RP}

since the length of RP is L\sqrt2.

And the gravitational force of attraction experienced by the mass placed at R due that at Q is also,

\displaystyle\longrightarrow F_Q=\dfrac{G}{2L^2}\ \sf{along\ RQ}

since the length of RQ is L\sqrt2.

Since RP=RQ=L\sqrt2 and PQ=2L, we see that \triangle PQR is a right triangle, right angled at R. So the net force acts along RO.

Hence the net gravitational force experienced by the mass placed at R due the two masses at P and Q is,

\displaystyle\longrightarrow\Sigma F=\sqrt{\left(F_P\right)^2+\left(F_Q\right)^2+2\cdot F_P\cdot F_Q\cos90^o}

\displaystyle\longrightarrow \Sigma F=\sqrt{\left(\dfrac{G}{2L^2}\right)^2+\left(\dfrac{G}{2L^2}\right)^2}

\longrightarrow\Sigma F=\sqrt{\dfrac{G^2}{4L^4}+\dfrac{G^2}{4L^4}}

\longrightarrow\underline{\underline{\Sigma F=\dfrac{G}{\sqrt2\,L^2}\ \sf{along\ RO}}}

Answered by Anonymous
33

Question:

Two particles each of mass 1kg are placed at P and Q such that PO=OQ=L.

The gravitational force experienced by another 1kg mass placed at R, where OR = L is

Theory :

⇒Newtons law of Gravitation

{\purple{\boxed{\large{\bold{F=\frac{Gm_{1}m_{2}}{r{}^{2}}}}}}}

Where , G = Universal gravitation constant

and r is distance between two Masses.

Solution :

Given : Two particles each of mass 1kg are placed at P and Q such that

PO=OQ=L and OR = L

we have to find The gravitational force experienced by another 1kg mass placed at R .

__________________________

PO=OQ=L and OR = L

⇒PR = RQ = √2L

 \bf F_{rp} =  \bf \frac{Gm {}^{2} }{( \sqrt{2}l) {}^{2} }  =\bf \frac{Gm {}^{2} }{2l {}^{2} }  = F

 \bf F_{rq} = \bf \frac{Gm {}^{2} }{ ( \sqrt{2}l) {}^{2}  }  = F

Now resultant of these forces

 \bf F_{net} =  \sqrt{F{}^{2} + F{}^{2}  }

 =  \sqrt{2} F

 =  \sqrt{2}  \times  \bf \frac{Gm {}^{2} }{2l {}^{2} }

 =  \bf \dfrac{Gm {}^{2}  }{ \sqrt{2}l {}^{2}  }

put m = 1 kg

 =  \bf \dfrac{G}{2l {}^{2} } \: along \: ro

correct option 1)

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