if a disc slides from the top to bottom of an inclined plane it takes time t1 If it rolls it takes time t2 now t2^2/t1^2
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t₁² = 2 L/(g SinФ) ; t₂² = 3 L/(g SinФ) => t₁² : t₂² = 2 : 3
Let the length of slope = L, mass of the disc = m.
Moment of Inertia about the center = I = MR² /2.
When the disc slides without rolling (when friction = 0):
a = g SinФ. u = 0, v = a t = g SinФ t
L = 1/2 g SinФ t₁² => t₁² = 2L/(g SinФ) ---(1)
When the disc rolls: friction ≠ 0.
Friction acts upwards along the point of contact. The disc rolls forward.
a = g sinФ - f/m => v = a t
Torque = I α = f R => R α = 2 f/m => ω = α t
Condition for Rolling: v = R ω or, a = R α
=> 3f/m = g sinФ => f = m g SinФ /3
We know f <= μ N or, μ m g CosΦ.
Hence, μ >= TanΦ /3 for the disc to roll. Otherwise, the disc only slides.
We assume that the time required from t = 0s, to when the disc starts rolling is very small.
=> a = g SinФ * 2/3
=> L = 1/2 *(g SinФ * 2/3 ) t₂²
=> t₂² = 3 L / (gSinФ)
Hence the ratio of squares of times to reach the floor: 2 : 3
Let the length of slope = L, mass of the disc = m.
Moment of Inertia about the center = I = MR² /2.
When the disc slides without rolling (when friction = 0):
a = g SinФ. u = 0, v = a t = g SinФ t
L = 1/2 g SinФ t₁² => t₁² = 2L/(g SinФ) ---(1)
When the disc rolls: friction ≠ 0.
Friction acts upwards along the point of contact. The disc rolls forward.
a = g sinФ - f/m => v = a t
Torque = I α = f R => R α = 2 f/m => ω = α t
Condition for Rolling: v = R ω or, a = R α
=> 3f/m = g sinФ => f = m g SinФ /3
We know f <= μ N or, μ m g CosΦ.
Hence, μ >= TanΦ /3 for the disc to roll. Otherwise, the disc only slides.
We assume that the time required from t = 0s, to when the disc starts rolling is very small.
=> a = g SinФ * 2/3
=> L = 1/2 *(g SinФ * 2/3 ) t₂²
=> t₂² = 3 L / (gSinФ)
Hence the ratio of squares of times to reach the floor: 2 : 3
kvnmurty:
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