Use numerical or graphical techniques to estimate the peak force of the collision in the preceding problem, and determine when it occurs. 82. During a crash test, a car moving at 50 km/h collides with a rigid barrier and comes to a complete stop in 200 ms. The collision force as a function of time is given by F = at 4 + bt 3 + ct 2 + dt , where a = −8.86GN/s 4 , b = 3.27 GN/s 3 , c = −362 MN/s 2 , and d = 12.5 MN/s. Find (a) the total impulse imparted by the collision, (b) the average collisional force, and (c) the car’s mass.
Use numerical or graphical techniques to estimate the peak force of the collision in the preceding problem, and determine when it occurs. 82. During a crash test, a car moving at 50 km/h collides with a rigid barrier and comes to a complete stop in 200 ms. The collision force as a function of time is given by F = at 4 + bt 3 + ct 2 + dt , where a = −8.86GN/s 4 , b = 3.27 GN/s 3 , c = −362 MN/s 2 , and d = 12.5 MN/s. Find (a) the total impulse imparted by the collision, (b) the average collisional force, and (c) the car’s mass.
Use numerical or graphical techniques to estimate the peak force of the collision in the preceding problem, and determine when it occurs.
82. During a crash test, a car moving at 50 km/h collides with a rigid barrier and comes to a complete stop in 200 ms. The collision force as a function of time is given by F = at4 + bt3 + ct2 + dt, where a = −8.86GN/s4, b = 3.27 GN/s3, c = −362 MN/s2, and d = 12.5 MN/s. Find (a) the total impulse imparted by the collision, (b) the average collisional force, and (c) the car’s mass.
Discuss the differences between the Biot-Savart law and Coulomb’s law in terms of their applicationsand the physical quantities they describe.
Explain why Ampere’s law can be used to find the magnetic field inside a solenoid but not outside.
3. An Atwood machine consists of two masses, mA
and m B, which are connected by an inelastic cord
of negligible mass that passes over a pulley. If the
pulley has radius RO and
moment of inertia I about its axle, determine the
acceleration of the masses
mA and m B, and compare to the situation where the
moment of inertia of the
pulley is ignored. Ignore friction at the axle O. Use
angular momentum and torque in this solution
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