An object with a mass of #14# # kg# is on a plane with an incline of # - pi/3 #. If it takes #12# # N# to start pushing the object down the plane and #7 # # N# to keep pushing it, what are the coefficients of static and kinetic friction?
Since the question doesn't specifically state it, we have to assume that once motion begins, it will always move at the same speed because that's the only explanation for the situation.
The sources of the forces will be:
For our purposes, we can disregard the negative sign in this instance because it simply indicates that the slope rises from right to left rather than from left to right.
The static friction expression is as follows:
Organizing:
While a little unusual, a frictional coefficient of 2 is not unheard of.
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To find the coefficients of static and kinetic friction, we can use the equations:
- ( F_{\text{friction, static}} = \mu_s \cdot N )
- ( F_{\text{friction, kinetic}} = \mu_k \cdot N )
Where:
- ( F_{\text{friction, static}} ) is the static friction force,
- ( F_{\text{friction, kinetic}} ) is the kinetic friction force,
- ( \mu_s ) is the coefficient of static friction,
- ( \mu_k ) is the coefficient of kinetic friction, and
- ( N ) is the normal force acting on the object.
First, let's find the normal force: [ N = mg \cos(\theta) ]
Given:
- Mass, ( m = 14 , \text{kg} )
- Incline angle, ( \theta = -\frac{\pi}{3} )
- Gravitational acceleration, ( g = 9.8 , \text{m/s}^2 )
[ N = (14 , \text{kg}) \times (9.8 , \text{m/s}^2) \times \cos\left(-\frac{\pi}{3}\right) ]
Now, we can use the given forces to find the coefficients of friction.
For static friction: [ F_{\text{friction, static}} = \mu_s \cdot N ] [ 12 , \text{N} = \mu_s \cdot N ]
For kinetic friction: [ F_{\text{friction, kinetic}} = \mu_k \cdot N ] [ 7 , \text{N} = \mu_k \cdot N ]
Dividing the equations: [ \frac{12 , \text{N}}{7 , \text{N}} = \frac{\mu_s \cdot N}{\mu_k \cdot N} ] [ \frac{12}{7} = \frac{\mu_s}{\mu_k} ] [ \mu_s = \frac{12}{7} \cdot \mu_k ]
Now, we need to find ( \mu_k ). [ \mu_k = \frac{7 , \text{N}}{N} ] [ \mu_k = \frac{7 , \text{N}}{14 , \text{kg} \times 9.8 , \text{m/s}^2 \times \cos\left(-\frac{\pi}{3}\right)} ]
Finally, we can substitute the value of ( \mu_k ) back into the equation for ( \mu_s ).
[ \mu_s = \frac{12}{7} \cdot \frac{7 , \text{N}}{14 , \text{kg} \times 9.8 , \text{m/s}^2 \times \cos\left(-\frac{\pi}{3}\right)} ]
Calculate the numerical values to find ( \mu_s ) and ( \mu_k ).
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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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