A box with an initial speed of #4 m/s# is moving up a ramp. The ramp has a kinetic friction coefficient of #5/6 # and an incline of #pi /4 #. How far along the ramp will the box go?

Answer 1

The distance is #=0.63ms^-1#

Taking the direction up and parallel to the plane as positive #↗^+#
The coefficient of kinetic friction is #mu_k=F_r/N#

Consequently, the object's net force is

#F=-F_r-Wsintheta#
#=-F_r-mgsintheta#
#=-mu_kN-mgsintheta#
#=mmu_kgcostheta-mgsintheta#

Newton's Second Law states

#F=m*a#
Where #a# is the acceleration So
#ma=-mu_kgcostheta-mgsintheta#
#a=-g(mu_kcostheta+sintheta)#
The coefficient of kinetic friction is #mu_k=5/6#
The incline of the ramp is #theta=1/4pi#
#a=-9.8*(5/6cos(1/4pi)+sin(1/4pi))#
#=-12.7ms^-2#

A deceleration is indicated by the negative sign.

We utilize the equation of motion.

#v^2=u^2+2as#
#u=4ms^-1#
#v=0#
#a=-12.7ms^-2#
#s=(v^2-u^2)/(2a)#
#=(0-16)/(-2*12.7)#
#=0.63m#
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Answer 2

To find the distance the box travels up the ramp, you can use the formula for the work done by friction:

[ W_{friction} = \mu_k \cdot m \cdot g \cdot d ]

Where: ( \mu_k ) = coefficient of kinetic friction (5/6 in this case) ( m ) = mass of the box ( g ) = acceleration due to gravity (approximately 9.8 m/s²) ( d ) = distance traveled up the ramp

You can also use the formula for gravitational force along the ramp:

[ F_{gravity} = m \cdot g \cdot \sin(\theta) ]

Where: ( \theta ) = angle of the incline (π/4 in this case)

Since the box is moving up the ramp, the force of friction opposes the gravitational force. Therefore:

[ W_{friction} = F_{gravity} ]

Solve for ( d ):

[ \mu_k \cdot m \cdot g \cdot d = m \cdot g \cdot \sin(\theta) ]

[ d = \frac{\sin(\theta)}{\mu_k} ]

Substitute the given values:

[ d = \frac{\sin(\frac{\pi}{4})}{\frac{5}{6}} ]

[ d = \frac{\frac{\sqrt{2}}{2}}{\frac{5}{6}} ]

[ d = \frac{6\sqrt{2}}{10} ]

[ d = \frac{3\sqrt{2}}{5} ]

So, the box will travel ( \frac{3\sqrt{2}}{5} ) meters along the ramp.

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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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