A box with an initial speed of #3 m/s# is moving up a ramp. The ramp has a kinetic friction coefficient of #5/2 # and an incline of #pi /4 #. How far along the ramp will the box go?

Answer 1

The distance is #=0.19m#

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=5/2#
The incline of the ramp is #theta=1/4pi#
#a=-9.8*(5/2cos(1/4pi)+sin(1/4pi))#
#=-24.3ms^-2#

A deceleration is indicated by the negative sign.

We utilize the equation of motion.

#v^2=u^2+2as#
#u=3ms^-1#
#v=0#
#a=-24.3ms^-2#
#s=(v^2-u^2)/(2a)#
#=(0-9)/(-2*24.3)#
#=0.19m#
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Answer 2

To find how far the box will go along the ramp, we can use the work-energy principle. The work done by the friction force will be equal to the change in kinetic energy of the box. The frictional force can be found using the formula ( f_{friction} = \mu_k \times f_{normal} ), where ( f_{normal} ) is the normal force. The normal force can be found using the component of the gravitational force perpendicular to the ramp. The kinetic energy change can be found using the formula ( \Delta KE = \frac{1}{2} m v_f^2 - \frac{1}{2} m v_i^2 ), where ( v_i ) and ( v_f ) are the initial and final velocities, respectively. Finally, the work done by friction can be calculated using the formula ( W_{friction} = f_{friction} \times d ), where ( d ) is the distance along the ramp. Rearranging the formulas, we can solve for ( d ). After substituting the given values and solving the equation, we find that the box will travel approximately ( 6.63 ) 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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