00. Scalar and Vector Quantities
Motion in Plane

143556 What is the torque of a force \(3 \hat{i}+7 \hat{j}+4 \hat{k}\) about the origin, if the force acts on a particle whose position vector is \(2 \hat{i}+2 \hat{j}+1 \hat{k}\) ?

1 \(\hat{i}-5 \hat{j}+8 \hat{k}\)
2 \(2 \hat{i}+2 \hat{j}+2 \hat{k}\)
3 \(\hat{i}+\hat{j}+\hat{k}\)
4 \(3 \hat{i}+2 \hat{j}+3 \hat{k}\)
Motion in Plane

143559 A certain vector in the \(x y\) plane has an \(x\) component of \(12 \mathrm{~m}\) and a y-component of \(8 \mathrm{~m}\). It is then rotated in the \(x y\) plane so that its \(x\) component is halved. Then its new \(y\) component is approximately

1 \(14 \mathrm{~m}\)
2 \(13.11 \mathrm{~m}\)
3 \(10 \mathrm{~m}\)
4 \(2.0 \mathrm{~m}\)
Motion in Plane

143560 Figure shows three forces \(\overrightarrow{\mathrm{F}}_{1}, \overrightarrow{\mathrm{F}}_{2}\) and \(\overrightarrow{\mathrm{F}}_{3}\) acting along the sides of an equilateral triangle. If the total torque acting at point ' \(O\) ' (centre of the triangle) is zero then the magnitude of \(\vec{F}_{3}\) is

1 \(\mathrm{F}_{1}+\mathrm{F}_{2}\)
2 \(\mathrm{F}_{1}-\mathrm{F}_{2}\)
3 \(\frac{\mathrm{F}_{1}-\mathrm{F}_{2}}{2}\)
4 \(\frac{\mathrm{F}_{1}}{\mathrm{~F}_{2}}\)
Motion in Plane

143561 Two forces each of magnitude ' \(P\) ' act at right angles. Their effect is neutralized by a third force acting along their bisector in opposite direction. The magnitude of the third force is \(\left[\cos \frac{\pi}{2}=0\right]\)

1 \(\mathrm{P}\)
2 \(\frac{\mathrm{P}}{\sqrt{2}}\)
3 \(\sqrt{2} \mathrm{P}\)
4 \(\frac{P}{2}\)
Motion in Plane

143556 What is the torque of a force \(3 \hat{i}+7 \hat{j}+4 \hat{k}\) about the origin, if the force acts on a particle whose position vector is \(2 \hat{i}+2 \hat{j}+1 \hat{k}\) ?

1 \(\hat{i}-5 \hat{j}+8 \hat{k}\)
2 \(2 \hat{i}+2 \hat{j}+2 \hat{k}\)
3 \(\hat{i}+\hat{j}+\hat{k}\)
4 \(3 \hat{i}+2 \hat{j}+3 \hat{k}\)
Motion in Plane

143559 A certain vector in the \(x y\) plane has an \(x\) component of \(12 \mathrm{~m}\) and a y-component of \(8 \mathrm{~m}\). It is then rotated in the \(x y\) plane so that its \(x\) component is halved. Then its new \(y\) component is approximately

1 \(14 \mathrm{~m}\)
2 \(13.11 \mathrm{~m}\)
3 \(10 \mathrm{~m}\)
4 \(2.0 \mathrm{~m}\)
Motion in Plane

143560 Figure shows three forces \(\overrightarrow{\mathrm{F}}_{1}, \overrightarrow{\mathrm{F}}_{2}\) and \(\overrightarrow{\mathrm{F}}_{3}\) acting along the sides of an equilateral triangle. If the total torque acting at point ' \(O\) ' (centre of the triangle) is zero then the magnitude of \(\vec{F}_{3}\) is

1 \(\mathrm{F}_{1}+\mathrm{F}_{2}\)
2 \(\mathrm{F}_{1}-\mathrm{F}_{2}\)
3 \(\frac{\mathrm{F}_{1}-\mathrm{F}_{2}}{2}\)
4 \(\frac{\mathrm{F}_{1}}{\mathrm{~F}_{2}}\)
Motion in Plane

143561 Two forces each of magnitude ' \(P\) ' act at right angles. Their effect is neutralized by a third force acting along their bisector in opposite direction. The magnitude of the third force is \(\left[\cos \frac{\pi}{2}=0\right]\)

1 \(\mathrm{P}\)
2 \(\frac{\mathrm{P}}{\sqrt{2}}\)
3 \(\sqrt{2} \mathrm{P}\)
4 \(\frac{P}{2}\)
Motion in Plane

143556 What is the torque of a force \(3 \hat{i}+7 \hat{j}+4 \hat{k}\) about the origin, if the force acts on a particle whose position vector is \(2 \hat{i}+2 \hat{j}+1 \hat{k}\) ?

1 \(\hat{i}-5 \hat{j}+8 \hat{k}\)
2 \(2 \hat{i}+2 \hat{j}+2 \hat{k}\)
3 \(\hat{i}+\hat{j}+\hat{k}\)
4 \(3 \hat{i}+2 \hat{j}+3 \hat{k}\)
Motion in Plane

143559 A certain vector in the \(x y\) plane has an \(x\) component of \(12 \mathrm{~m}\) and a y-component of \(8 \mathrm{~m}\). It is then rotated in the \(x y\) plane so that its \(x\) component is halved. Then its new \(y\) component is approximately

1 \(14 \mathrm{~m}\)
2 \(13.11 \mathrm{~m}\)
3 \(10 \mathrm{~m}\)
4 \(2.0 \mathrm{~m}\)
Motion in Plane

143560 Figure shows three forces \(\overrightarrow{\mathrm{F}}_{1}, \overrightarrow{\mathrm{F}}_{2}\) and \(\overrightarrow{\mathrm{F}}_{3}\) acting along the sides of an equilateral triangle. If the total torque acting at point ' \(O\) ' (centre of the triangle) is zero then the magnitude of \(\vec{F}_{3}\) is

1 \(\mathrm{F}_{1}+\mathrm{F}_{2}\)
2 \(\mathrm{F}_{1}-\mathrm{F}_{2}\)
3 \(\frac{\mathrm{F}_{1}-\mathrm{F}_{2}}{2}\)
4 \(\frac{\mathrm{F}_{1}}{\mathrm{~F}_{2}}\)
Motion in Plane

143561 Two forces each of magnitude ' \(P\) ' act at right angles. Their effect is neutralized by a third force acting along their bisector in opposite direction. The magnitude of the third force is \(\left[\cos \frac{\pi}{2}=0\right]\)

1 \(\mathrm{P}\)
2 \(\frac{\mathrm{P}}{\sqrt{2}}\)
3 \(\sqrt{2} \mathrm{P}\)
4 \(\frac{P}{2}\)
Motion in Plane

143556 What is the torque of a force \(3 \hat{i}+7 \hat{j}+4 \hat{k}\) about the origin, if the force acts on a particle whose position vector is \(2 \hat{i}+2 \hat{j}+1 \hat{k}\) ?

1 \(\hat{i}-5 \hat{j}+8 \hat{k}\)
2 \(2 \hat{i}+2 \hat{j}+2 \hat{k}\)
3 \(\hat{i}+\hat{j}+\hat{k}\)
4 \(3 \hat{i}+2 \hat{j}+3 \hat{k}\)
Motion in Plane

143559 A certain vector in the \(x y\) plane has an \(x\) component of \(12 \mathrm{~m}\) and a y-component of \(8 \mathrm{~m}\). It is then rotated in the \(x y\) plane so that its \(x\) component is halved. Then its new \(y\) component is approximately

1 \(14 \mathrm{~m}\)
2 \(13.11 \mathrm{~m}\)
3 \(10 \mathrm{~m}\)
4 \(2.0 \mathrm{~m}\)
Motion in Plane

143560 Figure shows three forces \(\overrightarrow{\mathrm{F}}_{1}, \overrightarrow{\mathrm{F}}_{2}\) and \(\overrightarrow{\mathrm{F}}_{3}\) acting along the sides of an equilateral triangle. If the total torque acting at point ' \(O\) ' (centre of the triangle) is zero then the magnitude of \(\vec{F}_{3}\) is

1 \(\mathrm{F}_{1}+\mathrm{F}_{2}\)
2 \(\mathrm{F}_{1}-\mathrm{F}_{2}\)
3 \(\frac{\mathrm{F}_{1}-\mathrm{F}_{2}}{2}\)
4 \(\frac{\mathrm{F}_{1}}{\mathrm{~F}_{2}}\)
Motion in Plane

143561 Two forces each of magnitude ' \(P\) ' act at right angles. Their effect is neutralized by a third force acting along their bisector in opposite direction. The magnitude of the third force is \(\left[\cos \frac{\pi}{2}=0\right]\)

1 \(\mathrm{P}\)
2 \(\frac{\mathrm{P}}{\sqrt{2}}\)
3 \(\sqrt{2} \mathrm{P}\)
4 \(\frac{P}{2}\)