Conservation of linear momentum/Galilean relativity problem

In summary, a conservation of linear momentum/Galilean relativity problem involves a 45-kg girl standing on a plank with a mass of 150 kg on a flat, frictionless surface. The girl begins to walk at a constant velocity of 1.5 m/s relative to the plank. The velocity of the plank relative to the ice surface is 0.346 m/s to the left, and the velocity of the girl relative to the ice surface is 1.15 m/s to the right. This is found by using the conservation of momentum equation and expressing the girl's velocity with respect to the ground in terms of the plank's velocity.
  • #1
NoPhysicsGenius
58
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[SOLVED] Conservation of linear momentum/Galilean relativity problem

Homework Statement




A 45-kg girl is standing on a plank that has a mass of 150 kg. The plank, originally at rest, is free to slide on a frozen lake, which is a flat, frictionless supporting surface. The girl begins to walk along the plank at a constant velocity of 1.5 m/s relative to the plank.

(a) What is her velocity relative to the ice surface?

(b) What is the velocity of the plank relative to the ice surface?


Homework Equations




[tex]m_1v_1 = m_2v_2[/tex]
[tex]\overrightarrow{p_{1i}} + \overrightarrow{p_{2i}} = \overrightarrow{p_{1f}} + \overrightarrow{p_{2f}}[/tex]

[tex]\overrightarrow{r}' = \overrightarrow{r} - \overrightarrow{u}t[/tex]
[tex]\overrightarrow{v}' = \overrightarrow{v} - \overrightarrow{u}[/tex]


The Attempt at a Solution




mass of girl:
[tex]m_g = 45 kg[/tex]

mass of plank:
[tex]m_p = 150 kg[/tex]

velocity of girl relative to plank:
[tex]v_{gp} = 1.5 m/s[/tex]

velocity of plank relative to girl:
[tex]v_{pg} = ?[/tex]

conservation of momentum:
[tex]m_gv_{gp} = m_pv_{pg} \Rightarrow[/tex]
[tex]v_{pg} = \frac{m_gv_{gp}}{m_p} = \frac{(45 kg)(1.5 m/s)}{150kg} = 0.450 m/s[/tex]


So I have the velocity of the plank relative to the girl; but I have no idea how to find the velocity of the girl or the plank relative to the ice. Can you help? Thank you.
 
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  • #2
I should also note that in the back of the book, the answer for (a) is 1.15 m/s and the answer for (b) is -0.346 m/s.
 
  • #3
v_pg and v_gp are equal and opposite in sign. They HAVE to be, just think about it. They are the same relative velocity measured in two different frames. You can't combine them in a single conservation of momentum equation. If vg and vp are the velocities relative to the ice, conservation of momentum tells you mg*vg+mp*vp=0. v_gp is just vg-vp.
 
  • #4
Dick said:
v_pg and v_gp are equal and opposite in sign. They HAVE to be, just think about it. They are the same relative velocity measured in two different frames. You can't combine them in a single conservation of momentum equation. If vg and vp are the velocities relative to the ice, conservation of momentum tells you mg*vg+mp*vp=0. v_gp is just vg-vp.

That makes sense. But now I'm really confused about how to proceed ...
 
  • #5
Just write an expression for conservation of momentum with all velocities with respect to the ground. The only unknown will be the velocity of the plank. Hint: Assume the plank goes left (negative) and the girl goes right (positive).
 
  • #6
Doc Al said:
Just write an expression for conservation of momentum with all velocities with respect to the ground. The only unknown will be the velocity of the plank.

How can the only unknown be the velocity of the plank? What is the velocity of the girl relative to the ground?
 
  • #7
You can express the girl's velocity with respect to the ground in terms of the plank's velocity.
 
  • #8
Now I get it! ...

[tex]v_{gi} = v_{gp} - v_{pi}[/tex]
[tex]m_gv_{gi} = m_pv_{pi}[/tex]
[tex]\Rightarrow m_g(v_{gp} - v_{pi}) = m_pv_{pi}[/tex]
[tex]\Rightarrow m_gv_{gp} - m_gv_{pi} = m_pv_{pi}[/tex]
[tex]\Rightarrow m_gv_{gp} = m_gv_{pi} + m_pv_{pi}[/tex]
[tex]\Rightarrow v_{pi} = \frac{m_gv_{gp}}{m_g + m_p}[/tex]
[tex]\Rightarrow v_{pi} = \frac{(45 kg)(1.50 m/s)}{45 kg + 150 kg} = 0.346 m/s[/tex]

So the velocity of the plank with respect to the ice is 0.346 m/s to the left. This is the answer for part (b).

To solve part (a) ...
[tex]v_{gi} = v_{gp} - v_{pi}[/tex]
[tex]\Rightarrow v_{gi} = 1.50 m/s - 0.346 m/s = 1.15 m/s (to the right)[/tex]

Thank you all for your time and patience! Especially Doc Al!
 

What is the conservation of linear momentum?

The conservation of linear momentum is a fundamental principle in physics that states that the total momentum of a closed system remains constant over time, unless there are external forces acting on the system. This means that the total momentum of all objects in the system before an event must equal the total momentum of all objects after the event.

How does the conservation of linear momentum relate to Galilean relativity?

The concept of Galilean relativity states that the laws of physics are the same in all inertial reference frames. This means that the conservation of linear momentum holds true in any inertial reference frame, regardless of its relative motion. In other words, the total momentum of a closed system will remain constant even if the reference frame is moving at a constant velocity.

What is an example of a conservation of linear momentum problem?

An example of a conservation of linear momentum problem is a collision between two objects. In this scenario, the total momentum of the two objects before the collision must equal the total momentum of the two objects after the collision, assuming there are no external forces acting on the system.

What are the limitations of the conservation of linear momentum?

The conservation of linear momentum only applies to closed systems, meaning that there are no external forces acting on the system. It also assumes that the system is in an inertial reference frame. Additionally, the conservation of linear momentum does not take into account any dissipative forces, such as friction, which can cause a decrease in the total momentum of the system.

How is the conservation of linear momentum used in real-world applications?

The conservation of linear momentum has many practical applications, including in the design of transportation systems, such as cars and airplanes. It is also used in sports, such as billiards and hockey, to predict the motion of objects after a collision. In addition, the principle is essential in the field of rocket science for calculating trajectories and orbits of spacecraft.

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