Determine is box of unknown mass is sliding down a ramp?

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SUMMARY

The discussion centers on determining whether a box of unknown mass will slide down a ramp inclined at 16 degrees, given a coefficient of static friction of 0.30 and kinetic friction of 0.25. The analysis reveals that the force driving the box down the ramp, represented by the component of gravitational force (Mgsin(16)), must exceed the opposing static friction force (µMgcos(16)) for sliding to occur. The conclusion is that the box will not slide down the ramp unless the angle is increased beyond a critical threshold where the gravitational force overcomes static friction.

PREREQUISITES
  • Understanding of Newton's second law (∑F=ma)
  • Knowledge of static and kinetic friction coefficients
  • Ability to resolve forces into components along an incline
  • Familiarity with trigonometric functions (sine and cosine) in physics
NEXT STEPS
  • Calculate the critical angle for sliding using the formula θ = arctan(µ).
  • Explore the effects of varying the angle of inclination on static and kinetic friction.
  • Investigate the relationship between mass and acceleration on inclined planes.
  • Learn about dynamics of motion on inclined planes, including forces and acceleration calculations.
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and forces, as well as educators seeking to explain concepts of friction and motion on inclined planes.

Jojo96
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Homework Statement


A box of textbooks at unknown mass rests on a loading ramp that makes an angle α = 16o with the horizontal. The coefficient of static friction is 0.30, and kinetic friction is 0.25. Then the box is released. (a) Will it start sliding down the ramp? (a) Find the normal force on the box (b) If it slides down then find the acceleration of the box

2. Relevant
F=ma
ƒ=µn

The Attempt at a Solution


Forces in x-direction:
w-ƒstatic=0
w=ƒstatic
mgsin(16)=µn
y: n-w=0
n=w
n=mgcos(16)
------
mgsin(16)=µmgcos(16)
sin(16)=µcos(16)
sin(16)/cos(16)=µ
But already know µ so this doesn't help me...
[/B]
 
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By assuming ##\sum F_x=0## you're stating that the block isn't moving in the x direction. Try using ##\sum F_x=ma_x##
 
Jojo96 said:
3. The Attempt at a Solution
Forces in x-direction:
w-ƒstatic=0
w=ƒstatic
mgsin(16)=µn
y: n-w=0
n=w
n=mgcos(16)
------
mgsin(16)=µmgcos(16)
sin(16)=µcos(16)
sin(16)/cos(16)=µ
But already know µ so this doesn't help me...

with the ramp at your angle theta - if you calculate the force driving the box then perhaps it will come out less than the frictional force opposing the tendency to slide down- as it will be mu. M.g .cos (angle)
 
The only force that is driving it down is the weight. Nothing is pulling the box. Also, what would I use for acceleration in the x direction for F=ma?
 
Jojo96 said:
The only force that is driving it down is the weight. Nothing is pulling the box. Also, what would I use for acceleration in the x direction for F=ma?
Component of weight along the slope is pulling the box down. Check if it is sufficient to overcome static friction.
 
Jojo96 said:
The only force that is driving it down is the weight. Nothing is pulling the box. Also, what would I use for acceleration in the x direction for F=ma?

along the ramp the force acting downward will be component of Mg - i.e. Mg sin(16)- but your body can not move with this pull along the ramp as frictional force is larger - if you increase the angle of ramp then only it can move at an angle Theta such that Mgsin(theta) exceeds
(Coeff. of friction XMg Cos(theta)) which is opposing the motion acting along the ramp in upward direction.
 

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