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1000 small water drops each of radius 'r' and charge 'q' coalesce together to one spherical drop. The potential of the big drop is larger than that of the smaller drops by
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![tan^-1 [ cos x1 + sin x ] is equal to](https://dwes9vv9u0550.cloudfront.net/images/3616471/165cccf1-7df9-468e-aa5d-ceeb0aec94a7.jpg "tan^-1 [ cos x1 + sin x ] is equal to")
tan^-1 [ cos x1 + sin x ] is equal to
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![a) = −i dt (d − 3) 2 Γ 2 [ d−3 2 ] 128(d − 2) 2 π d−1 | Download Scientific Diagram](https://www.researchgate.net/publication/23503561/figure/fig1/AS:588227446603779@1517255760835/Fig3a-i-dt-d-3-2-G-2-d-3-2-128d-2-2-p-d-1.png "a) = −i dt (d − 3) 2 Γ 2 [ d−3 2 ] 128(d − 2) 2 π d−1 | Download Scientific Diagram")
a) = −i dt (d − 3) 2 Γ 2 [ d−3 2 ] 128(d − 2) 2 π d−1 | Download Scientific Diagram
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Formulas 2 - Section Properties（Area , Section Modulus , Moment of Inertia , Radius of Gyration） Structural calculation, strength of materials
A lamina of mass $M$ in the shape of a quarter of the disc of radius $R$ as shown in figure. The moment of inertia of this lamina about axis $AB$ is (
Formulas 1 - Section Properties（Area , Section Modulus , Moment of Inertia , Radius of Gyration） Structural calculation, strength of materials
Formulas 1 - Section Properties（Area , Section Modulus , Moment of Inertia , Radius of Gyration） Structural calculation, strength of materials
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