00. Centre of Mass
Rotational Motion

269492 A circular hole of radius '\(r\) ' is made in a disk of radius ' \(R\) ' and of uniform thickness at a distance ' \(a\) ' from the centre of the disk. The distance of the new centre of mass from the original centre of mass is
">

1 \(\frac{a R^{2}}{R^{2}-r^{2}}\)
2 \(\frac{a r^{2}}{R^{2}-r^{2}}\)
3 \(\frac{a\left(R^{2}-r^{2}\right)}{r^{2}}\)
4 \(\frac{a\left(R^{2}-r^{2}\right)}{R^{2}}\)
Rotational Motion

269493 Thecentre of mass of the letter \(F\) which is cut from a uniform metal sheet from point \(A\) is

1 \(15 / 7,33 / 7\)
2 \(15 / 7,23 / 7\)
3 \(22 / 7,33 / 7\)
4 \(33 / 7,22 / 7\)
Rotational Motion

269494 Two identical thin uniform rods of length\(L\) each are joined to form \(T\) shape as shown in the figure. The distance of centre of mass from \(D\) is

1 0
2 \(\mathrm{L} / 4\)
3 \(3 \mathrm{~L} / 4\)
4 \(\mathrm{L}\)
Rotational Motion

269495 Figure shows a square plate of uniform thickness and side length\(\sqrt{2} \mathrm{~m}\). One fourth of the plate is removed as indicated. The distance of centre of mass of the remaining portion from the centre of the original square plate is

1 \(1 / 3 \mathrm{~m}\)
2 \(1 / 2 \mathrm{~m}\)
3 \(1 / 6 \mathrm{~m}\)
4 \(1 / 8 \mathrm{~m}\)
Rotational Motion

269545 Four particles, each of mass \(1 \mathrm{~kg}\), are placed at the comers of square of side one meter in the XY plane. If the point of intersection of the diagonals of the square is taken as the origin,the co-ordinates of the center of mass are

1 \((1,1)\)
2 \((-1,1)\)
3 \((1,-1)\)
4 \((0,0)\)
Rotational Motion

269492 A circular hole of radius '\(r\) ' is made in a disk of radius ' \(R\) ' and of uniform thickness at a distance ' \(a\) ' from the centre of the disk. The distance of the new centre of mass from the original centre of mass is
">

1 \(\frac{a R^{2}}{R^{2}-r^{2}}\)
2 \(\frac{a r^{2}}{R^{2}-r^{2}}\)
3 \(\frac{a\left(R^{2}-r^{2}\right)}{r^{2}}\)
4 \(\frac{a\left(R^{2}-r^{2}\right)}{R^{2}}\)
Rotational Motion

269493 Thecentre of mass of the letter \(F\) which is cut from a uniform metal sheet from point \(A\) is

1 \(15 / 7,33 / 7\)
2 \(15 / 7,23 / 7\)
3 \(22 / 7,33 / 7\)
4 \(33 / 7,22 / 7\)
Rotational Motion

269494 Two identical thin uniform rods of length\(L\) each are joined to form \(T\) shape as shown in the figure. The distance of centre of mass from \(D\) is

1 0
2 \(\mathrm{L} / 4\)
3 \(3 \mathrm{~L} / 4\)
4 \(\mathrm{L}\)
Rotational Motion

269495 Figure shows a square plate of uniform thickness and side length\(\sqrt{2} \mathrm{~m}\). One fourth of the plate is removed as indicated. The distance of centre of mass of the remaining portion from the centre of the original square plate is

1 \(1 / 3 \mathrm{~m}\)
2 \(1 / 2 \mathrm{~m}\)
3 \(1 / 6 \mathrm{~m}\)
4 \(1 / 8 \mathrm{~m}\)
Rotational Motion

269545 Four particles, each of mass \(1 \mathrm{~kg}\), are placed at the comers of square of side one meter in the XY plane. If the point of intersection of the diagonals of the square is taken as the origin,the co-ordinates of the center of mass are

1 \((1,1)\)
2 \((-1,1)\)
3 \((1,-1)\)
4 \((0,0)\)
Rotational Motion

269492 A circular hole of radius '\(r\) ' is made in a disk of radius ' \(R\) ' and of uniform thickness at a distance ' \(a\) ' from the centre of the disk. The distance of the new centre of mass from the original centre of mass is
">

1 \(\frac{a R^{2}}{R^{2}-r^{2}}\)
2 \(\frac{a r^{2}}{R^{2}-r^{2}}\)
3 \(\frac{a\left(R^{2}-r^{2}\right)}{r^{2}}\)
4 \(\frac{a\left(R^{2}-r^{2}\right)}{R^{2}}\)
Rotational Motion

269493 Thecentre of mass of the letter \(F\) which is cut from a uniform metal sheet from point \(A\) is

1 \(15 / 7,33 / 7\)
2 \(15 / 7,23 / 7\)
3 \(22 / 7,33 / 7\)
4 \(33 / 7,22 / 7\)
Rotational Motion

269494 Two identical thin uniform rods of length\(L\) each are joined to form \(T\) shape as shown in the figure. The distance of centre of mass from \(D\) is

1 0
2 \(\mathrm{L} / 4\)
3 \(3 \mathrm{~L} / 4\)
4 \(\mathrm{L}\)
Rotational Motion

269495 Figure shows a square plate of uniform thickness and side length\(\sqrt{2} \mathrm{~m}\). One fourth of the plate is removed as indicated. The distance of centre of mass of the remaining portion from the centre of the original square plate is

1 \(1 / 3 \mathrm{~m}\)
2 \(1 / 2 \mathrm{~m}\)
3 \(1 / 6 \mathrm{~m}\)
4 \(1 / 8 \mathrm{~m}\)
Rotational Motion

269545 Four particles, each of mass \(1 \mathrm{~kg}\), are placed at the comers of square of side one meter in the XY plane. If the point of intersection of the diagonals of the square is taken as the origin,the co-ordinates of the center of mass are

1 \((1,1)\)
2 \((-1,1)\)
3 \((1,-1)\)
4 \((0,0)\)
Rotational Motion

269492 A circular hole of radius '\(r\) ' is made in a disk of radius ' \(R\) ' and of uniform thickness at a distance ' \(a\) ' from the centre of the disk. The distance of the new centre of mass from the original centre of mass is
">

1 \(\frac{a R^{2}}{R^{2}-r^{2}}\)
2 \(\frac{a r^{2}}{R^{2}-r^{2}}\)
3 \(\frac{a\left(R^{2}-r^{2}\right)}{r^{2}}\)
4 \(\frac{a\left(R^{2}-r^{2}\right)}{R^{2}}\)
Rotational Motion

269493 Thecentre of mass of the letter \(F\) which is cut from a uniform metal sheet from point \(A\) is

1 \(15 / 7,33 / 7\)
2 \(15 / 7,23 / 7\)
3 \(22 / 7,33 / 7\)
4 \(33 / 7,22 / 7\)
Rotational Motion

269494 Two identical thin uniform rods of length\(L\) each are joined to form \(T\) shape as shown in the figure. The distance of centre of mass from \(D\) is

1 0
2 \(\mathrm{L} / 4\)
3 \(3 \mathrm{~L} / 4\)
4 \(\mathrm{L}\)
Rotational Motion

269495 Figure shows a square plate of uniform thickness and side length\(\sqrt{2} \mathrm{~m}\). One fourth of the plate is removed as indicated. The distance of centre of mass of the remaining portion from the centre of the original square plate is

1 \(1 / 3 \mathrm{~m}\)
2 \(1 / 2 \mathrm{~m}\)
3 \(1 / 6 \mathrm{~m}\)
4 \(1 / 8 \mathrm{~m}\)
Rotational Motion

269545 Four particles, each of mass \(1 \mathrm{~kg}\), are placed at the comers of square of side one meter in the XY plane. If the point of intersection of the diagonals of the square is taken as the origin,the co-ordinates of the center of mass are

1 \((1,1)\)
2 \((-1,1)\)
3 \((1,-1)\)
4 \((0,0)\)
Rotational Motion

269492 A circular hole of radius '\(r\) ' is made in a disk of radius ' \(R\) ' and of uniform thickness at a distance ' \(a\) ' from the centre of the disk. The distance of the new centre of mass from the original centre of mass is
">

1 \(\frac{a R^{2}}{R^{2}-r^{2}}\)
2 \(\frac{a r^{2}}{R^{2}-r^{2}}\)
3 \(\frac{a\left(R^{2}-r^{2}\right)}{r^{2}}\)
4 \(\frac{a\left(R^{2}-r^{2}\right)}{R^{2}}\)
Rotational Motion

269493 Thecentre of mass of the letter \(F\) which is cut from a uniform metal sheet from point \(A\) is

1 \(15 / 7,33 / 7\)
2 \(15 / 7,23 / 7\)
3 \(22 / 7,33 / 7\)
4 \(33 / 7,22 / 7\)
Rotational Motion

269494 Two identical thin uniform rods of length\(L\) each are joined to form \(T\) shape as shown in the figure. The distance of centre of mass from \(D\) is

1 0
2 \(\mathrm{L} / 4\)
3 \(3 \mathrm{~L} / 4\)
4 \(\mathrm{L}\)
Rotational Motion

269495 Figure shows a square plate of uniform thickness and side length\(\sqrt{2} \mathrm{~m}\). One fourth of the plate is removed as indicated. The distance of centre of mass of the remaining portion from the centre of the original square plate is

1 \(1 / 3 \mathrm{~m}\)
2 \(1 / 2 \mathrm{~m}\)
3 \(1 / 6 \mathrm{~m}\)
4 \(1 / 8 \mathrm{~m}\)
Rotational Motion

269545 Four particles, each of mass \(1 \mathrm{~kg}\), are placed at the comers of square of side one meter in the XY plane. If the point of intersection of the diagonals of the square is taken as the origin,the co-ordinates of the center of mass are

1 \((1,1)\)
2 \((-1,1)\)
3 \((1,-1)\)
4 \((0,0)\)