An object with a mass of #12 kg# is revolving around a point at a distance of #12 m#. If the object is making revolutions at a frequency of #1 Hz#, what is the centripetal force acting on the object?
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The centripetal force acting on the object can be calculated using the formula:
(F = m \cdot r \cdot \omega^2)
Where: (F) = centripetal force, (m) = mass of the object, (r) = radius of the circular path, (\omega) = angular velocity.
Given: (m = 12 \text{ kg}), (r = 12 \text{ m}), Frequency (f = 1 \text{ Hz}).
Angular velocity ((\omega)) can be calculated as (2\pi f).
Substituting the values:
(\omega = 2\pi \cdot 1 = 2\pi \text{ rad/s})
(F = 12 \text{ kg} \cdot 12 \text{ m} \cdot (2\pi)^2 \text{ rad/s}^2)
(F \approx 144 \pi^2 \text{ N} \approx 1423.72 \text{ N})
Therefore, the centripetal force acting on the object is approximately (1423.72 \text{ N}).
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The centripetal force acting on the object can be calculated using the formula:
[ F = m \times r \times \omega^2 ]
Where:
- ( F ) is the centripetal force,
- ( m ) is the mass of the object,
- ( r ) is the distance from the object to the center of rotation,
- ( \omega ) is the angular velocity, which is ( 2\pi ) times the frequency (( f )).
Given that ( m = 12 ) kg, ( r = 12 ) m, and ( f = 1 ) Hz, we can calculate ( \omega ):
[ \omega = 2\pi \times f = 2\pi \times 1 = 2\pi , \text{rad/s} ]
Now, substituting the values into the formula:
[ F = 12 \times 12 \times (2\pi)^2 = 288 \pi^2 , \text{N} ]
Therefore, the centripetal force acting on the object is ( 288 \pi^2 ) N.
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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