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sattari [20]
3 years ago
13

1.How does inertia affect a person who is not wearing a seatbelt during a collision?

Physics
1 answer:
natali 33 [55]3 years ago
8 0
1) Inertia is the tendency of an object in motion to keep moving in straight line with constant velocity, or to remain at rest if the object was initially at rest. A person in a moving car is moving together with the car, so his inertia is his tendency to keep moving with constant velocity. During a collision, therefore, if the person is not wearing a seatbelt, he will continue to move forrward due to his inertia (while the car will stop due to the crash), and eventually he will hit the windscreen of the car.

2) The more the kinetic energy, the larger the distance needed to stop the car. In fact, calling vi the initial speed of the car, vf the final velocity (which is zero, because we want the car to stop), a the deceleration of the car and S the stopping distance, we can use the following relationship:
v_f^2-v_i^2=2aS
Since vf=0, we can rewrite the stopping distance as
S=- \frac{v_i^2}{2a}
The vehicle in the two situations is the same, so we see that the larger the initial velocity (which means more kinetic energy), the larger the stopping distance. In particular, in this case the velocity in the second situation (60 mph) is twice the velocity in the first situation (30 mph), so the stopping distance in the second situation is 2^2=4 times larger than in the first situation.

3) The large vehicle has a larger mass than the small vehicle, so it also has greater kinetic energy, which is given by:
K= \frac{1}{2} mv^2
where m is the mass of the car and v is its velocity. Due to its larger mass, the large vehicle has a greater inertia: it means it would take more effort to stop it. In fact, the work done to stop the car is W=FS, where F is the force of the brakes and S is the stopping distance. For the work-energy theorem, this work is equal to the initial kinetic energy of the car:
\frac{1}{2} mv^2=FS
If we assume the brakes in the two cars can apply the same force, then we see that the larger the mass m, the larger the stopping distance S.

4) The best way for the driver to prepare to enter the sharp curve is to decrease the velocity: in fact, decreasing the velocity (and so, decreasing the kinetic energy) will allow him to stay in the curved path more easily. If the car is going too fast, it will tend to go straight away (due to its inertia), and it won't be able to do the curve.

<span>5) The damages produced by a car crash depend on the energy involved in the accident: the more the energy released, the larger the damages. In particular, since we are talking about kinetic energy
</span>K= \frac{1}{2} mv^2<span>
we see that the larger the mass of the vehicle, the greater the energy involved and so the larger the damages; and similarly, the larger the speed of the vehicle v, the greater the energy involved and so the larger the damages of the car crash.</span>
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3 years ago
Under the influence of its drive force, a snowmobile is moving at a constant velocity along a horizontal patch of snow. When the
balandron [24]

Answer:

a) Δx = 11.6 m

b) t = 3.9 s

Explanation:

a)

  • Since the snowmobile is moving at constant speed, and the drive force is 195 N, this means that thereis another force equal and opposite acting on it, according to Newton's 2nd Law, due to there is no acceleration present in the horizontal direction .
  • This force is just the force of kinetic friction, and is equal to -195 N (assuming the positive direction as the direction of the movement).
  • Once the drive force is shut off, the only force acting on the snowmobile remains the friction force.
  • According Newton's 2nd Law, this force is causing a negative acceleration (actually slowing down the snowmobile) that can be found as follows:

       a = \frac{F_{fr} }{m} = \frac{-195N}{128kg} = -1.5 m/s2 (1)

  • Assuming the friction force keeps constant, we can use the following kinematic equation in order to find the distance traveled under this acceleration before coming to an stop, as follows:

       v_{f} ^{2}  -v_{o} ^{2} = 2* a* \Delta x (2)

  • Taking into account that vf=0, replacing by the given (v₀) and a from (1), we can solve for Δx, as follows:

       \Delta x =- \frac{v_{o}^{2}}{2*a} =- \frac{(5.90m/s)^{2}}{2*(-1.5m/s2)} = 11.6 m (3)

b)

  • We can find the time needed to come to an stop, applying the definition of acceleration, as follows:

       v_{f} = v_{o} + a*\Delta t (4)

  • Since we have already said that the snowmobile comes to an stop, this means that vf = 0.
  • Replacing a and v₀ as we did in (3), we can solve for Δt as follows:

       \Delta t = \frac{-v_{o} }{a} = \frac{-5.9m/s}{-1.5m/s2} = 3.9 s   (5)

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jolli1 [7]

Answer:

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