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Linear speed refers to how fast an object moves along the path of its motion. When dealing with a rotating object, like a drill bit, the maximum linear speed typically occurs at the perimeter or edge of the object. Imagine you're on a merry-go-round: the farther you are from the center, the faster you're moving in relation to the ground. A similar concept applies to rotating objects.
To calculate the linear speed of a point on the edge of a drill bit, you can use the formula:

• \( v = \omega r \)

Here, \( v \) is the linear speed, \( \omega \) is the angular speed, and \( r \) is the radius of the circle traced out by the edge of the bit. In our case, the drill bit has a diameter of \(12.7\, \mathrm{mm}\), so its radius is half of that: \(0.00635\, \mathrm{m}\).
Given the angular speed \(\omega = 130.9\, \text{rad/s}\), the linear speed \( v \) comes out to about \(0.831\, \text{m/s}\). This means the edge of the bit moves at a speed of \(0.831\, \text{m/s}\) relative to the center of the circle it makes as it spins.

Radial acceleration, also known as centripetal acceleration, is the rate of change of velocity directed towards the center of the circular path. This is crucial because without this inward force, the rotating object would fly off in a straight line due to inertia. Imagine twirling a stone tied to a string; the tension in the string provides the centripetal force pulling the stone towards your hand.
For a rotating drill bit, the maximum radial acceleration can be calculated using:

• \( a_c = \omega^2 r \)

In this formula, \( \omega \) is the angular speed, and \( r \) is the radius of the circular path followed by the drill bit's edge. By substituting \( \omega = 130.9\, \text{rad/s} \) and \( r = 0.00635\, \mathrm{m} \), the radial acceleration \( a_c \) is approximately \( 108.9\, \text{m/s}^2 \).
This high value shows how much acceleration is needed to keep the edge of the drill bit rotating in its circular path, preventing it from moving off in a tangent.

Angular speed describes how quickly an object rotates or revolves relative to another point, usually the center of rotation. It's like the speedometer for rotational motion, measuring how fast an object goes around a circle.
In rotational motion, angular speed is denoted by \( \omega \) and is measured in radians per second \(\text{rad/s}\). This differs from linear speed, which measures how fast an object moves along a path. The relationship between the two in circular motion is given by:

• \( \omega = \frac{v}{r} \)
• \( v = \omega r \) (for linear speed)

For our drill bit, the angular speed was initially given as \( 1250\, \text{rev/min} \). After converting revolutions per minute to radians per second, we find \( \omega \approx 130.9 \text{rad/s} \). This conversion is crucial because radians are the standard unit in physics for measuring rotation angles.
Understanding angular speed is vital, as it helps determine other important quantities like linear speed and radial acceleration, ultimately allowing us to better grasp the dynamics of rotating objects.