A box with an initial speed of #7 m/s# is moving up a ramp. The ramp has a kinetic friction coefficient of #7/3 # and an incline of #(5 pi )/12 #. How far along the ramp will the box go?
The distance is
Consequently, the object's net force is
Newton's Second Law states
So
A deceleration is indicated by the negative sign.
We utilize the equation of motion.
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To find how far along the ramp the box will go, we can use the equations of motion and the principles of physics. First, we'll calculate the acceleration of the box up the ramp using the components of the gravitational force and the frictional force. Then, we'll use the kinematic equation to find the distance traveled.
The acceleration up the ramp can be found using the following equation:
[ a = g \sin(\theta) - \mu_k g \cos(\theta) ]
where ( g ) is the acceleration due to gravity, ( \theta ) is the angle of the incline, and ( \mu_k ) is the coefficient of kinetic friction.
Given:
- ( g = 9.8 , \text{m/s}^2 ) (acceleration due to gravity)
- ( \theta = \frac{5\pi}{12} )
- ( \mu_k = \frac{7}{3} )
Substituting the values, we get:
[ a = (9.8 , \text{m/s}^2) \sin\left(\frac{5\pi}{12}\right) - \left(\frac{7}{3}\right)(9.8 , \text{m/s}^2) \cos\left(\frac{5\pi}{12}\right) ]
Then we find:
[ a ≈ -5.978 , \text{m/s}^2 ]
The negative sign indicates that the acceleration is acting in the opposite direction to the motion of the box.
Now, we can use the equation of motion to find the distance traveled:
[ d = v_i t + \frac{1}{2} a t^2 ]
Where:
- ( v_i ) is the initial velocity (7 m/s)
- ( t ) is the time
- ( a ) is the acceleration
Since the box eventually comes to rest, its final velocity ( v_f = 0 ). We can use this information to find the time taken (( t )):
[ v_f = v_i + at ] [ 0 = 7 - 5.978t ] [ t ≈ 1.17 , \text{s} ]
Now, plug this time value into the equation to find the distance traveled:
[ d = (7 , \text{m/s})(1.17 , \text{s}) + \frac{1}{2}(-5.978 , \text{m/s}^2)(1.17 , \text{s})^2 ] [ d ≈ 5.56 , \text{m} ]
So, the box will travel approximately 5.56 meters along the ramp before coming to rest.
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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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