An object with a mass of #6 kg# is on a plane with an incline of # - pi/6 #. If it takes #18 N# to start pushing the object down the plane and #1 N# to keep pushing it, what are the coefficients of static and kinetic friction?
Now that we have our prerequisites, let's start by thinking about the static case.
When we solve, we
Examining the kinetic scenario first
When we solve, we obtain
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The coefficient of static friction is μs = 0.577 and the coefficient of kinetic friction is μk = 0.100.
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The force required to start pushing the object down the plane is the force of static friction, ( F_s ). The force required to keep pushing it once it's in motion is the force of kinetic friction, ( F_k ).
The force of static friction is given by:
[ F_s = \mu_s \cdot N ]
where ( \mu_s ) is the coefficient of static friction and ( N ) is the normal force.
The normal force ( N ) is equal to the gravitational force acting perpendicular to the plane, which is ( mg \cos(\theta) ), where ( m ) is the mass of the object, ( g ) is the acceleration due to gravity, and ( \theta ) is the angle of the incline.
Given:
- ( m = 6 ) kg
- ( g \approx 9.8 ) m/s² (acceleration due to gravity)
- ( \theta = -\frac{\pi}{6} )
We have: [ N = mg \cos(\theta) = 6 \times 9.8 \times \cos\left(-\frac{\pi}{6}\right) ]
The force of kinetic friction ( F_k ) is given by:
[ F_k = \mu_k \cdot N ]
where ( \mu_k ) is the coefficient of kinetic friction.
Given that it takes 18 N to start pushing the object down the plane and 1 N to keep pushing it, we have:
[ F_s = 18 \text{ N} ] [ F_k = 1 \text{ N} ]
We can now solve for ( \mu_s ) and ( \mu_k ) using the formulas for static and kinetic friction.
[ \mu_s = \frac{F_s}{N} ] [ \mu_k = \frac{F_k}{N} ]
After calculating ( N ), ( \mu_s ), and ( \mu_k ), we'll have the coefficients of static and kinetic friction.
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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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