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alekssr [168]
3 years ago
14

You are designing an amusement park ride. A cart with two riders moves horizontally with speed v = 5.40 m/s . You assume that th

e total mass of cart plus riders is 300 kg. The cart hits a light spring that is attached to a wall, momentarily comes to rest as the spring is compressed, and then regains speed as it moves back in the opposite direction. For the ride to be thrilling but safe, the maximum acceleration of the cart during this motion should be 3.00g. Ignore friction. what is
(a) the required force constant of the bring
(b) the maximun distance the spring will be compressed.
Physics
1 answer:
jok3333 [9.3K]3 years ago
5 0

Answer:

Spring constant required=8910 N/m.  Maximum distance compressed=0.99m

Explanation:

The first step here is to consider the Newton's Second Law which states that a force <em>F</em> applied to a body of mass <em>m</em> produces an acceleration <em>a</em>. Our body has a mass of 300 kg and the maximum allowable acceleration is 3.00 g. Considering gravity g=9.81m/s^2, <em>a</em>=3.00*9.81m/s^=29.43m/s^2. Hence,

F=300kg*29.43 m/s^2=8829 N

The force that a spring gives is the multiplication of its force constant <em>K </em>and the distance compressed<em> X.</em> . So the force F sholud be equal to <em>K*X_{max}. </em>

<em>F=K*X_{max}.</em>

Then, when the spring is fully compressed all the kinetic energy of the cart (T) is transferred to the spring as potential elastic energy (U). <em> </em>

<em>1/2*m*v^2=1/2*K*X_{max}^2  Eq.1</em>

We do not know X_{max} but we do know that it is equal to F/<em>K. </em>Thus,

1/2*m*v^2=1/2*K*(\frac{F}{K} )^{2} Eq.2

Operating in Eq.2 K=(\frac{F}{v} )^{2} \frac{1}{m}=8910.75 N/m

Finally, putting the valus of <em>K </em>in Eq.1 and solving, <em>X_{max}=0.99m</em>

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(a) No, because the mechanical energy is not conserved

Explanation:

The work-energy theorem states that the work done by the engine on the airplane is equal to the gain in kinetic energy of the plane:

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However, this theorem is only valid if there are no non-conservative forces acting on the plane. However, in this case there is air resistance acting on the plane: this means that the work-energy theorem is no longer valid, because the mechanical energy is not conserved.

Therefore, eq. (1) can be rewritten as

W=\Delta K + E_{lost}

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(b) 77.8 m/s

First of all, we need to calculate the net force acting on the plane, which is equal to the difference between the thrust force and the air resistance:

F=7.70\cdot 10^4 N - 5.00 \cdot 10^4 N=2.70\cdot 10^4 N

Now we can calculate the acceleration of the plane, by using Newton's second law:

a=\frac{F}{m}=\frac{2.70\cdot 10^4 N}{1.60\cdot 10^4 kg}=1.69 m/s^2

where m is the mass of the plane.

Finally, we can calculate the final speed of the plane by using the equation:

v^2- u^2 = 2aS

where

v=? is the final velocity

u=66.0 m/s is the initial velocity

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<u>Friction Force</u>

When objects are in contact with other objects or rough surfaces, the friction forces appear when we try to move them with respect to each other. The friction forces always have a direction opposite to the intended motion, i.e. if the object is pushed to the right, the friction force is exerted to the left.

There are two blocks, one of 400 kg on a horizontal surface and other of 100 kg on top of it tied to a vertical wall by a string. If we try to push the first block, it will not move freely, because two friction forces appear: one exerted by the surface and the other exerted by the contact between both blocks. Let's call them Fr1 and Fr2 respectively. The block 2 is attached to the wall by a string, so it won't simply move with the block 1.  

Please find the free body diagrams in the figure provided below.

The equilibrium condition for the mass 1 is

\displaystyle F_a-F_{r1}-F_{r2}=m.a=0

The mass m1 is being pushed by the force Fa so that slipping with the mass m2 barely occurs, thus the system is not moving, and a=0. Solving for Fa

\displaystyle F_a=F_{r1}+F_{r2}.....[1]

The mass 2 is tried to be pushed to the right by the friction force Fr2 between them, but the string keeps it fixed in position with the tension T. The equation in the horizontal axis is

\displaystyle F_{r2}-T=0

The friction forces are computed by

\displaystyle F_{r2}=\mu \ N_2=\mu\ m_2\ g

\displaystyle F_{r1}=\mu \ N_1=\mu(m_1+m_2)g

Recall N1 is the reaction of the surface on mass m1 which holds a total mass of m1+m2.

Replacing in [1]

\displaystyle F_{a}=\mu \ m_2\ g\ +\mu(m_1+m_2)g

Simplifying

\displaystyle F_{a}=\mu \ g(m_1+2\ m_2)

Plugging in the values

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