Chapter 5: Problem 13
Why might your car start to skid if you drive too fast around a curve?
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These are the key concepts you need to understand to accurately answer the question.
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Chapter 5: Problem 13
Why might your car start to skid if you drive too fast around a curve?
These are the key concepts you need to understand to accurately answer the question.
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Suppose the drag force acting on a freefalling object is proportional to the velocity. The net force acting on the object would be \(F=m g-b v\). (a) Using dimensional analysis, determine the units of the constant \(b\). (b) Find an expression for velocity as a function of time for the object.
In a weird parallel universe, an object moving through a liquid experiences a drag force proportional to the inverse of the object's speed, that is, \(F_{\mathrm{drag}}=-b v^{-1}\). (a) An object of mass \(m\) has an initial speed \(v_{0}\) in the liquid. Derive an equation which gives the speed as a function of time. (b) An object enters the liquid with an initial speed \(10 \mathrm{~m} / \mathrm{s}\), and after \(9 \mathrm{~s}\) its speed is \(8 \mathrm{~m} / \mathrm{s}\). Determine the time it takes for the object to come to a complete stop. In both cases the drag force is the only force on the object. SSM
The terminal velocity of a raindrop that is \(4.0\) \(\mathrm{mm}\) in diameter is approximately \(8.5 \mathrm{~m} / \mathrm{s}\) under controlled, windless conditions. The density of water is \(1000 \mathrm{~kg} / \mathrm{m}^{3}\). Recall that the density of an object is its mass divided by its volume. (a) If we model the air drag as being proportional to the square of the speed, \(F_{\mathrm{drag}}=-b v^{2}\), what is the value of \(b\) ? (b) Under the same conditions as above, what would be the terminal velocity of a raindrop that is \(8.0 \mathrm{~mm}\) in diameter? Try to use your answer from part (a) to solve the problem by proportional reasoning instead of just doing the same calculation over again.
A 25 -g metal washer is tied to a 60 -cm-long string and whirled around in a vertical circle at a constant speed of \(6 \mathrm{~m} / \mathrm{s}\). Calculate the tension in the string (a) when the washer is at the bottom of the circular path and (b) when it is at the top of the path.
A hockey puck that has a mass of \(170 \mathrm{~g}\) is tied to a light string and spun in a circle of radius \(1.25 \mathrm{~m}\) (on frictionless ice). If the string breaks under a tension that exceeds \(5.00 \mathrm{~N}\), at what angular speed (revolutions per minute) will the string break?
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