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 #2 Hz#, what is the centripetal force acting on the object?

Answer 1

I found: #7580N#

Centripetal Force is: #F_c=mv^2/r# where: #m=#mass; #v=# linear velocity; #r=# radius.
The frequency tells us the number of complete revolutions in one seconds (here 2 revolutions). We can ask ourselves what will be the Angular Velocity #omega# of our object, i.e., a kind of "curved" velocity involving not linear distance but angle described in time!

So we get:

#omega="angle"/"time"=(2pi)/T#
Where #T# will be the Period of time for a complete revolution (time to describe #2pi# radians).
The good thing is that the period is connected to frequency as #"frequency"=nu=1/T# and also the angular velocity can be changed into linear velocity simply considering at what distance from the center you are travelling....(basically, you include the radius)!!!! so: #v=omega*r#

in our case we get (collecting all our stuff):

#F_c=m(omega*r)^2/r=momega^2r=m(2pinu)^2r=6*(2*3.14*2)^2*8~~7580N#
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Answer 2

The centripetal force acting on the object is 192 N.

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Answer from HIX Tutor

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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