Momentum, Force and Inertia
LAWS OF MOTION (ADDITIONAL)

371687 Three forces \(A=(i+j+k), B=(2 i-j+3 k)\) and \(C\) acting on a body to keep it in equilibrium. Then \(C\) is

1 \(-(3 \mathrm{i}+4 \mathrm{k})\)
2 \(-(4 \mathrm{i}+3 \mathrm{k})\)
3 \(3 \mathrm{i}+4 \mathrm{j}\)
4 \(2 \mathrm{i}-3 \mathrm{k}\)
LAWS OF MOTION (ADDITIONAL)

371688 A mass \(m\) falls freely from rest. The linear momentum, after it has fallen through a height \(h\), is :
( \(g\) = acceleration due to gravity)

1 \(\sqrt{\mathrm{mgh}}\)
2 \(\mathrm{m} \sqrt{2 g h}\)
3 \(\mathrm{m} \sqrt{\mathrm{gh}}\)
4 zero
LAWS OF MOTION (ADDITIONAL)

371689 Two masses of \(\mathrm{m}\) and \(4 \mathrm{~m}\) are moving with equal kinetic energy. The ratio of their linear momentum is

1 \(1: 8\)
2 \(1: 4\)
3 \(1: 2\)
4 \(4: 1\)
LAWS OF MOTION (ADDITIONAL)

371690 The one which does not represent a force in any context is

1 friction
2 impulse
3 tension
4 weight
5 viscous drag
LAWS OF MOTION (ADDITIONAL)

371687 Three forces \(A=(i+j+k), B=(2 i-j+3 k)\) and \(C\) acting on a body to keep it in equilibrium. Then \(C\) is

1 \(-(3 \mathrm{i}+4 \mathrm{k})\)
2 \(-(4 \mathrm{i}+3 \mathrm{k})\)
3 \(3 \mathrm{i}+4 \mathrm{j}\)
4 \(2 \mathrm{i}-3 \mathrm{k}\)
LAWS OF MOTION (ADDITIONAL)

371688 A mass \(m\) falls freely from rest. The linear momentum, after it has fallen through a height \(h\), is :
( \(g\) = acceleration due to gravity)

1 \(\sqrt{\mathrm{mgh}}\)
2 \(\mathrm{m} \sqrt{2 g h}\)
3 \(\mathrm{m} \sqrt{\mathrm{gh}}\)
4 zero
LAWS OF MOTION (ADDITIONAL)

371689 Two masses of \(\mathrm{m}\) and \(4 \mathrm{~m}\) are moving with equal kinetic energy. The ratio of their linear momentum is

1 \(1: 8\)
2 \(1: 4\)
3 \(1: 2\)
4 \(4: 1\)
LAWS OF MOTION (ADDITIONAL)

371690 The one which does not represent a force in any context is

1 friction
2 impulse
3 tension
4 weight
5 viscous drag
LAWS OF MOTION (ADDITIONAL)

371687 Three forces \(A=(i+j+k), B=(2 i-j+3 k)\) and \(C\) acting on a body to keep it in equilibrium. Then \(C\) is

1 \(-(3 \mathrm{i}+4 \mathrm{k})\)
2 \(-(4 \mathrm{i}+3 \mathrm{k})\)
3 \(3 \mathrm{i}+4 \mathrm{j}\)
4 \(2 \mathrm{i}-3 \mathrm{k}\)
LAWS OF MOTION (ADDITIONAL)

371688 A mass \(m\) falls freely from rest. The linear momentum, after it has fallen through a height \(h\), is :
( \(g\) = acceleration due to gravity)

1 \(\sqrt{\mathrm{mgh}}\)
2 \(\mathrm{m} \sqrt{2 g h}\)
3 \(\mathrm{m} \sqrt{\mathrm{gh}}\)
4 zero
LAWS OF MOTION (ADDITIONAL)

371689 Two masses of \(\mathrm{m}\) and \(4 \mathrm{~m}\) are moving with equal kinetic energy. The ratio of their linear momentum is

1 \(1: 8\)
2 \(1: 4\)
3 \(1: 2\)
4 \(4: 1\)
LAWS OF MOTION (ADDITIONAL)

371690 The one which does not represent a force in any context is

1 friction
2 impulse
3 tension
4 weight
5 viscous drag
LAWS OF MOTION (ADDITIONAL)

371687 Three forces \(A=(i+j+k), B=(2 i-j+3 k)\) and \(C\) acting on a body to keep it in equilibrium. Then \(C\) is

1 \(-(3 \mathrm{i}+4 \mathrm{k})\)
2 \(-(4 \mathrm{i}+3 \mathrm{k})\)
3 \(3 \mathrm{i}+4 \mathrm{j}\)
4 \(2 \mathrm{i}-3 \mathrm{k}\)
LAWS OF MOTION (ADDITIONAL)

371688 A mass \(m\) falls freely from rest. The linear momentum, after it has fallen through a height \(h\), is :
( \(g\) = acceleration due to gravity)

1 \(\sqrt{\mathrm{mgh}}\)
2 \(\mathrm{m} \sqrt{2 g h}\)
3 \(\mathrm{m} \sqrt{\mathrm{gh}}\)
4 zero
LAWS OF MOTION (ADDITIONAL)

371689 Two masses of \(\mathrm{m}\) and \(4 \mathrm{~m}\) are moving with equal kinetic energy. The ratio of their linear momentum is

1 \(1: 8\)
2 \(1: 4\)
3 \(1: 2\)
4 \(4: 1\)
LAWS OF MOTION (ADDITIONAL)

371690 The one which does not represent a force in any context is

1 friction
2 impulse
3 tension
4 weight
5 viscous drag