Newton's Law of Motion and It's Application
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LAWS OF MOTION (ADDITIONAL)

371765 Consider a ship traveling due east along the equator with velocity \(v_{0}\). If southeastern wind blows at an angle of ' \(\phi\) ' to the equator with velocity ' \(v\) '. The wind velocity relative to the ship \(v^{\prime}\) and the angle between the equator and the wind direction in the reference frame fixed to the slip are

1 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v} \sin \phi}{\mathrm{v}^{\prime}}\right)\)
2 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{vv}_{0} \sin \phi}, \cos ^{-1}\left(\frac{\mathrm{v} \cos \phi}{\mathrm{v}^{\prime}}\right)\)
3 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
4 \(\mathrm{v}^{\prime}=\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi, \cos ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
TS EAMCET 02.05.2018
LAWS OF MOTION (ADDITIONAL)

371766 \(90 \mathrm{~N}\) mass is hung on a rope tied between two poles as shown in the figure. The tension \(T_{1}\) and \(T_{2}\) in the two parts of the rope are (in \(N\) ).

1 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}+1}\)
2 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}}\)
3 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}+1}\)
4 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}}\)
TS EAMCET (Medical)-02.05.2018
LAWS OF MOTION (ADDITIONAL)

371767 If a stone of mass \(0.05 \mathrm{~kg}\) is thrown out a window of a train moving at a constant speed of \(100 \mathrm{~km} / \mathrm{h}\) then magnitude of the net force acting on the stone is

1 \(0.5 \mathrm{~N}\)
2 zero
3 \(50 \mathrm{~N}\)
4 \(5 \mathrm{~N}\)
BITSAT-2018
LAWS OF MOTION (ADDITIONAL)

371768 A lift moves vertically up with an acceleration a. Force exerted by a person of mass \(M\) on the floor of the lift is

1 \(\mathrm{Ma}\)
2 \(\mathrm{Mg}\)
3 \(\mathrm{M}(\mathrm{g}+\mathrm{a})\)
4 \(M(g-a)\)
J and K-CET-2017
LAWS OF MOTION (ADDITIONAL)

371769 Consider the following statements in the context of forjmulation of any law of Physics
I. explain the existing physical facts
II. no need of experimental verification
III. predict future results
Then, any formulated law of Physics, should be true with respect to:

1 I and II
2 II and III
3 I and III
4 I,II and III
TS EAMCET(Medical)-2017
NEET DIGITAL LIBRARY
LAWS OF MOTION (ADDITIONAL)

371765 Consider a ship traveling due east along the equator with velocity \(v_{0}\). If southeastern wind blows at an angle of ' \(\phi\) ' to the equator with velocity ' \(v\) '. The wind velocity relative to the ship \(v^{\prime}\) and the angle between the equator and the wind direction in the reference frame fixed to the slip are

1 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v} \sin \phi}{\mathrm{v}^{\prime}}\right)\)
2 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{vv}_{0} \sin \phi}, \cos ^{-1}\left(\frac{\mathrm{v} \cos \phi}{\mathrm{v}^{\prime}}\right)\)
3 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
4 \(\mathrm{v}^{\prime}=\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi, \cos ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
TS EAMCET 02.05.2018
LAWS OF MOTION (ADDITIONAL)

371766 \(90 \mathrm{~N}\) mass is hung on a rope tied between two poles as shown in the figure. The tension \(T_{1}\) and \(T_{2}\) in the two parts of the rope are (in \(N\) ).

1 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}+1}\)
2 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}}\)
3 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}+1}\)
4 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}}\)
TS EAMCET (Medical)-02.05.2018
LAWS OF MOTION (ADDITIONAL)

371767 If a stone of mass \(0.05 \mathrm{~kg}\) is thrown out a window of a train moving at a constant speed of \(100 \mathrm{~km} / \mathrm{h}\) then magnitude of the net force acting on the stone is

1 \(0.5 \mathrm{~N}\)
2 zero
3 \(50 \mathrm{~N}\)
4 \(5 \mathrm{~N}\)
BITSAT-2018
LAWS OF MOTION (ADDITIONAL)

371768 A lift moves vertically up with an acceleration a. Force exerted by a person of mass \(M\) on the floor of the lift is

1 \(\mathrm{Ma}\)
2 \(\mathrm{Mg}\)
3 \(\mathrm{M}(\mathrm{g}+\mathrm{a})\)
4 \(M(g-a)\)
J and K-CET-2017
LAWS OF MOTION (ADDITIONAL)

371769 Consider the following statements in the context of forjmulation of any law of Physics
I. explain the existing physical facts
II. no need of experimental verification
III. predict future results
Then, any formulated law of Physics, should be true with respect to:

1 I and II
2 II and III
3 I and III
4 I,II and III
TS EAMCET(Medical)-2017
Join With Us for More Updates
LAWS OF MOTION (ADDITIONAL)

371765 Consider a ship traveling due east along the equator with velocity \(v_{0}\). If southeastern wind blows at an angle of ' \(\phi\) ' to the equator with velocity ' \(v\) '. The wind velocity relative to the ship \(v^{\prime}\) and the angle between the equator and the wind direction in the reference frame fixed to the slip are

1 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v} \sin \phi}{\mathrm{v}^{\prime}}\right)\)
2 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{vv}_{0} \sin \phi}, \cos ^{-1}\left(\frac{\mathrm{v} \cos \phi}{\mathrm{v}^{\prime}}\right)\)
3 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
4 \(\mathrm{v}^{\prime}=\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi, \cos ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
TS EAMCET 02.05.2018
LAWS OF MOTION (ADDITIONAL)

371766 \(90 \mathrm{~N}\) mass is hung on a rope tied between two poles as shown in the figure. The tension \(T_{1}\) and \(T_{2}\) in the two parts of the rope are (in \(N\) ).

1 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}+1}\)
2 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}}\)
3 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}+1}\)
4 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}}\)
TS EAMCET (Medical)-02.05.2018
LAWS OF MOTION (ADDITIONAL)

371767 If a stone of mass \(0.05 \mathrm{~kg}\) is thrown out a window of a train moving at a constant speed of \(100 \mathrm{~km} / \mathrm{h}\) then magnitude of the net force acting on the stone is

1 \(0.5 \mathrm{~N}\)
2 zero
3 \(50 \mathrm{~N}\)
4 \(5 \mathrm{~N}\)
BITSAT-2018
LAWS OF MOTION (ADDITIONAL)

371768 A lift moves vertically up with an acceleration a. Force exerted by a person of mass \(M\) on the floor of the lift is

1 \(\mathrm{Ma}\)
2 \(\mathrm{Mg}\)
3 \(\mathrm{M}(\mathrm{g}+\mathrm{a})\)
4 \(M(g-a)\)
J and K-CET-2017
LAWS OF MOTION (ADDITIONAL)

371769 Consider the following statements in the context of forjmulation of any law of Physics
I. explain the existing physical facts
II. no need of experimental verification
III. predict future results
Then, any formulated law of Physics, should be true with respect to:

1 I and II
2 II and III
3 I and III
4 I,II and III
TS EAMCET(Medical)-2017
For More Updates join with Us
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LAWS OF MOTION (ADDITIONAL)

371765 Consider a ship traveling due east along the equator with velocity \(v_{0}\). If southeastern wind blows at an angle of ' \(\phi\) ' to the equator with velocity ' \(v\) '. The wind velocity relative to the ship \(v^{\prime}\) and the angle between the equator and the wind direction in the reference frame fixed to the slip are

1 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v} \sin \phi}{\mathrm{v}^{\prime}}\right)\)
2 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{vv}_{0} \sin \phi}, \cos ^{-1}\left(\frac{\mathrm{v} \cos \phi}{\mathrm{v}^{\prime}}\right)\)
3 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
4 \(\mathrm{v}^{\prime}=\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi, \cos ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
TS EAMCET 02.05.2018
LAWS OF MOTION (ADDITIONAL)

371766 \(90 \mathrm{~N}\) mass is hung on a rope tied between two poles as shown in the figure. The tension \(T_{1}\) and \(T_{2}\) in the two parts of the rope are (in \(N\) ).

1 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}+1}\)
2 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}}\)
3 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}+1}\)
4 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}}\)
TS EAMCET (Medical)-02.05.2018
LAWS OF MOTION (ADDITIONAL)

371767 If a stone of mass \(0.05 \mathrm{~kg}\) is thrown out a window of a train moving at a constant speed of \(100 \mathrm{~km} / \mathrm{h}\) then magnitude of the net force acting on the stone is

1 \(0.5 \mathrm{~N}\)
2 zero
3 \(50 \mathrm{~N}\)
4 \(5 \mathrm{~N}\)
BITSAT-2018
LAWS OF MOTION (ADDITIONAL)

371768 A lift moves vertically up with an acceleration a. Force exerted by a person of mass \(M\) on the floor of the lift is

1 \(\mathrm{Ma}\)
2 \(\mathrm{Mg}\)
3 \(\mathrm{M}(\mathrm{g}+\mathrm{a})\)
4 \(M(g-a)\)
J and K-CET-2017
LAWS OF MOTION (ADDITIONAL)

371769 Consider the following statements in the context of forjmulation of any law of Physics
I. explain the existing physical facts
II. no need of experimental verification
III. predict future results
Then, any formulated law of Physics, should be true with respect to:

1 I and II
2 II and III
3 I and III
4 I,II and III
TS EAMCET(Medical)-2017
NEET DIGITAL LIBRARY
LAWS OF MOTION (ADDITIONAL)

371765 Consider a ship traveling due east along the equator with velocity \(v_{0}\). If southeastern wind blows at an angle of ' \(\phi\) ' to the equator with velocity ' \(v\) '. The wind velocity relative to the ship \(v^{\prime}\) and the angle between the equator and the wind direction in the reference frame fixed to the slip are

1 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v} \sin \phi}{\mathrm{v}^{\prime}}\right)\)
2 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}+2 \mathrm{vv}_{0} \sin \phi}, \cos ^{-1}\left(\frac{\mathrm{v} \cos \phi}{\mathrm{v}^{\prime}}\right)\)
3 \(\mathrm{v}^{\prime}=\sqrt{\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi}, \sin ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
4 \(\mathrm{v}^{\prime}=\mathrm{v}_{0}^{2}+\mathrm{v}^{2}-2 \mathrm{v}_{0} \mathrm{v} \cos \phi, \cos ^{-1}\left(\frac{\mathrm{v}}{\mathrm{v}^{\prime}}\right)\)
TS EAMCET 02.05.2018
LAWS OF MOTION (ADDITIONAL)

371766 \(90 \mathrm{~N}\) mass is hung on a rope tied between two poles as shown in the figure. The tension \(T_{1}\) and \(T_{2}\) in the two parts of the rope are (in \(N\) ).

1 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}+1}\)
2 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{6}}{2}, \frac{180}{\sqrt{3}}\)
3 \(\frac{180}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}+1}\)
4 \(\frac{90}{\sqrt{3}+1} \cdot \frac{\sqrt{3}}{2}, \frac{90}{\sqrt{3}}\)
TS EAMCET (Medical)-02.05.2018
LAWS OF MOTION (ADDITIONAL)

371767 If a stone of mass \(0.05 \mathrm{~kg}\) is thrown out a window of a train moving at a constant speed of \(100 \mathrm{~km} / \mathrm{h}\) then magnitude of the net force acting on the stone is

1 \(0.5 \mathrm{~N}\)
2 zero
3 \(50 \mathrm{~N}\)
4 \(5 \mathrm{~N}\)
BITSAT-2018
LAWS OF MOTION (ADDITIONAL)

371768 A lift moves vertically up with an acceleration a. Force exerted by a person of mass \(M\) on the floor of the lift is

1 \(\mathrm{Ma}\)
2 \(\mathrm{Mg}\)
3 \(\mathrm{M}(\mathrm{g}+\mathrm{a})\)
4 \(M(g-a)\)
J and K-CET-2017
LAWS OF MOTION (ADDITIONAL)

371769 Consider the following statements in the context of forjmulation of any law of Physics
I. explain the existing physical facts
II. no need of experimental verification
III. predict future results
Then, any formulated law of Physics, should be true with respect to:

1 I and II
2 II and III
3 I and III
4 I,II and III
TS EAMCET(Medical)-2017