From conservation of mechanical energy at top and bottom point of inclined plane:
→ mgh = 1/2 mv² ( 1+ k²/ r²)
hence, v =
also, v²=u² +2as
a= v² /2s
a= 2gh/ (1+ k²/r²) 2s
now, h/s =sinQ (qetha)
hence, a =gsinQ/ 1+k²/r²
now, as its a sphere therefore, k²/r² = 2/5
hence, a= 5/7 gsinQ
-frictional force is given by: ma * k²/r²
therefore, f = m* 5/7 gsinQ * 2/5
∴ f= 2/7 mg sinQ
- for the sphere to roll without slip, limiting friction should be greater than the applied frictonal force :
f ≤
2/7mgsinQ ≤ ∪R
2/7gsinQ ≤ ∪gcosQ (R=mgcosQ ; ∪ =coeffecient of friction)
2/7tanQ, ≤ ∪
hence,
= 2/7 tanQ
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Hey there!From conservation of mechanical energy at top and bottom point of inclined plane:
→ mgh = 1/2 mv² ( 1+ k²/ r²)
hence, v =
also, v²=u² +2as
a= v² /2s
a= 2gh/ (1+ k²/r²) 2s
now, h/s =sinQ (qetha)
hence, a =gsinQ/ 1+k²/r²
now, as its a sphere therefore, k²/r² = 2/5
hence, a= 5/7 gsinQ
-frictional force is given by: ma * k²/r²
therefore, f = m* 5/7 gsinQ * 2/5
∴ f= 2/7 mg sinQ
- for the sphere to roll without slip, limiting friction () should be greater than the applied frictonal force :
f ≤
2/7mgsinQ ≤ ∪R
2/7gsinQ ≤ ∪gcosQ (R=mgcosQ ; ∪ =coeffecient of friction)
2/7tanQ ≤ ∪
hence, = 2/7 tanQ
# HOPE THE ANSWER HELPS!
From conservation of mechanical energy at top and bottom point of inclined plane:
→ mgh = 1/2 mv² ( 1+ k²/ r²)
hence, v =
also, v²=u² +2as
a= v² /2s
a= 2gh/ (1+ k²/r²) 2s
now, h/s =sinQ (qetha)
hence, a =gsinQ/ 1+k²/r²
now, as its a sphere therefore, k²/r² = 2/5
hence, a= 5/7 gsinQ
-frictional force is given by: ma * k²/r²
therefore, f = m* 5/7 gsinQ * 2/5
∴ f= 2/7 mg sinQ
- for the sphere to roll without slip, limiting friction should be greater than the applied frictonal force :
f ≤
2/7mgsinQ ≤ ∪R
2/7gsinQ ≤ ∪gcosQ (R=mgcosQ ; ∪ =coeffecient of friction)
2/7tanQ, ≤ ∪
hence,
= 2/7 tanQ