An object with a mass of #6 kg# is revolving around a point at a distance of #8 m#. If the object is making revolutions at a frequency of #6 Hz#, what is the centripetal force acting on the object?
The force acting on the object is
We'll start by determining the velocity of the object. Since it is revolving in a circle of radius 8m 6 times per second, we know that:
Plugging in values gives us:
Now we can use the standard equation for centripetal acceleration:
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The centripetal force acting on an object in circular motion can be calculated using the formula:
[ F_c = m \times r \times (2\pi f)^2 ]
where ( m ) is the mass of the object, ( r ) is the radius of the circular path, and ( f ) is the frequency of revolutions.
Substituting the given values:
[ F_c = 6 , \text{kg} \times 8 , \text{m} \times (2\pi \times 6 , \text{Hz})^2 ]
[ F_c = 6 , \text{kg} \times 8 , \text{m} \times (2\pi \times 6)^2 , \text{Hz}^2 ]
[ F_c = 6 , \text{kg} \times 8 , \text{m} \times (36\pi^2) , \text{Hz}^2 ]
[ F_c = 1728 \pi^2 , \text{N} ]
So, the centripetal force acting on the object is ( 1728 \pi^2 , \text{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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