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Concept explainers
A crash test is performed between an SUV A and a 2500-lb compact car B. The compact car is stationary before the impact and has its brakes applied. A transducer measures the force during the impact, and the force P varies as shown. Knowing that the coefficients of friction between the tires and road are
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(a)
The time at which the compact car starts moving.
Answer to Problem 13.137P
Time at which the compact car starts moving
Explanation of Solution
Given information:
Weight of compact car B is equal to
“A force acting on a particle during a very short time interval but large enough to produce a definite change in momentum is called an impulsive force.”
Impulse momentum principle for impulsive motion is defined as:
Calculation:
Apply impulse momentum principle.
Substitute,
Find Friction force,
The force during impact P varies,
At
Substitute in equation 1:
Conclusion:
The time when the compact car starts moving is calculated by putting the values of the weight of the car and friction force in the momentum principle equation.
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(b)
The maximum speed of the car
Answer to Problem 13.137P
Explanation of Solution
Given information:
Weight of compact car B is equal to
“A force acting on a particle during a very short time interval but large enough to produce a definite change in momentum is called an impulsive force.”
Impulse momentum principle for impulsive motion is defined as,
Calculation:
Find the friction factor when moving,
At
But we know that,
Apply impulse momentum principle,
Substitute,
Therefore,
Conclusion:
The maximum speed is equal to
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(c)
The time at which car comes to stop
Answer to Problem 13.137P
Explanation of Solution
Given information:
Weight of compact car B is equal to
“A force acting on a particle during a very short time interval but large enough to produce a definite change in momentum is called an impulsive force.”
Impulse momentum principle for impulsive motion is defined as,
Calculation:
To find the stopping time,
Apply impulse momentum principle,
Therefore,
Conclusion:
The car comes to stop at
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Chapter 13 Solutions
Vector Mechanics for Engineers: Dynamics
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