Time and Date Stamps (logged): 01:32:08 08-29-2008 ¯°Ÿ²±Ÿ¯·¯·Ÿ±¸Ÿ±¯¯· Precalculus II

General College Physics (Phy 201) Test 2


Completely document your work and your reasoning.

You will be graded on your documentation, your reasoning, and the correctness of your conclusions.


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Instructions:

Directions for Student:

Test Problems:

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Problem Number 1

Sketch a force diagram depicting weight and normal force for a glider gliding down an inclined air track. Indicate an x axis parallel to the incline and a y axis perpendicularto the x axis. Sketch the force vectors to scale and indicate their x and y components. Also sketch the net force vector, in the appropriate direction and also to scale.

Sketch a diagram to show the forces that would result if a horizontal force equal to half the weight of the glider was exerted in a direction that would tend to push the glider up the incline. Indicate the x and y components of all these vectors. Sketch all vectors and all components to scale.

We know that for an air cart gliding along an incline, the force that accelerates it is equal to W sin(`theta), where W is the weight of the cart and `theta the angle of the incline with horizontal.

If the force on the glider was W, what would be its acceleration?

If the acceleration of a mass is proportional to the net force acting on it, then

what should be the acceleration of the glider under the influence of a net force of .04 W?

what should be the acceleration of the glider under the influence of net force W sin(`theta)?

What should be the acceleration of the glider for `theta = 3 degrees?

What is the slope of the incline corresponding to this angle?

Explain why, for small angles, acceleration is proportional to slope.

 

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Problem Number 2

What is the gravitational field strength of Earth at a distance of 2.3 Earth radii from center?  Solve in two ways:

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Problem Number 3

Explain why the work required to stretch a spring or other elastic object with a linear restoring force, of form F = - kx, from its equilibrium position to displacement x is `dW = .5 k x^2, and why we hence say that this is the elastic potential energy of the object in this position.

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Problem Number 4

A uniform sphere of mass .71 kg and radius 23 cm is constrained to rotate on an axis about its center. Friction exerts a net torque of .0004232 meter Newtons on the system when it is in motion. On the disk are mounted masses of 21 grams at a distance of 16.1 cm from the axis of rotation, 14 grams data distance of 13.34 cm from the axis and 47 grams at a distance of 8.51 cm from the axis. A uniform force of .008 Newtons is applied at the rim of the sphere at 23 cm from the axis of rotation.

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Problem Number 5

If a mass of 7 kg moving at 4 m/s collides with a mass of 7 kg moving at -4 m/s, and the two masses are 'stuck together' after collision, then what is their common velocity after collision?  Is this collision possible for the system consisting of the two masses without the conversion of some internal source of potential energy?

 

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Problem Number 6

A neutron star might have about five times the mass of our Sun, around 10^31 kg, packed into a very nearly perfect sphere of radius roughly 10 km.  If you suddenly appeared at the surface of a Neutron star you would almost instantly become a part of that nearly perfect sphere (though you would probably be integrated nearer to your point of contact, you might think of yourself as almost instantly forming a thin coat, like a coat of paint, over the surface of the star). 

Suppose you somehow managed to retain your mass and some form of structural integrity and began walking across the surface of the star.