Laws of Motion
- A block A of mass m1 rests on a horizontal table. A light string connected to it passes over a frictionless pulley at the edge of table and from its other end another block B of mass m2 is suspended. The coefficient of kinetic friction between the block and the table is µk. When the block A is sliding on the table, the tension in the string is
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NA
Correct Option: D
NA
- Consider a car moving along a straight horizontal road with a speed of 72 km/h. If the coefficient of static friction between the tyres and the road is 0.5, the shortest distance in which the car can be stopped is (taking g = 10 m/s²)
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Here u = 72 km/h = 20 m/s; v = 0;
a = – µg = – 0.5 × 10 = – 5 m/s²
As v² = u² + 2as,∴ s = (v² - u²) = (0 - (20)²) = 40 m 2a 2 × (-5)
Correct Option: B
Here u = 72 km/h = 20 m/s; v = 0;
a = – µg = – 0.5 × 10 = – 5 m/s²
As v² = u² + 2as,∴ s = (v² - u²) = (0 - (20)²) = 40 m 2a 2 × (-5)
- A heavy uniform chain lies on horizontal table top. If the coefficient of friction between the chain and the table surface is 0.25, then the maximum fraction of the length of the chain that can hang over one edge of the table is
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The force of friction on the chain lying on the table should be equal to the weight of the hanging chain. Let
ρ = mass per unit length of the chain
µ = coefficient of friction
l = length of the total chain
x = length of hanging chain
Now, µ(l – x) ρg = xρg or µ(l – x) = x
or µl = (µ + 1)x or x = µl/(µ + 1)∴ x = 0.25l = 0.25l = 0.2l (0.25 + 1) 1.25 x = 0.2 = 20% l
Correct Option: A
The force of friction on the chain lying on the table should be equal to the weight of the hanging chain. Let
ρ = mass per unit length of the chain
µ = coefficient of friction
l = length of the total chain
x = length of hanging chain
Now, µ(l – x) ρg = xρg or µ(l – x) = x
or µl = (µ + 1)x or x = µl/(µ + 1)∴ x = 0.25l = 0.25l = 0.2l (0.25 + 1) 1.25 x = 0.2 = 20% l
- Starting from rest, a body slides down a 45° inclined plane in twice the time it takes to slide down the same distance in the absence of friction. The coefficient of friction between the body and the inclined plane is
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In presence of friction a = (g sinθ – µg cos θ)
∴ Time taken to slide down the planet1 = √ 2s = √ 2s = 48 a g(sinθ - μ cosθ) In absence of friction t2 = √ 2s g sinθ
t1 2t2
&there; t1² 4t2²or = 2s = 2s × 4 g(sinθ - μcosθ) gsinθ
sin θ = 4 sinθ – 4µ cos θμ = 3 tanθ = 3 = 0.75 4 4
Correct Option: B
In presence of friction a = (g sinθ – µg cos θ)
∴ Time taken to slide down the planet1 = √ 2s = √ 2s = 48 a g(sinθ - μ cosθ) In absence of friction t2 = √ 2s g sinθ
t1 2t2
&there; t1² 4t2²or = 2s = 2s × 4 g(sinθ - μcosθ) gsinθ
sin θ = 4 sinθ – 4µ cos θμ = 3 tanθ = 3 = 0.75 4 4
- A car is negotiating a curved road of radius R. The road is banked at an angle θ. the coefficient of friction between the tyres of the car and the road is µs. The maximum safe velocity on this road is :
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On a banked road,
Vmax² = μs + tanθ Rg 1 - μs tanθ
Maximum safe velocity of a car on the banked roadVmax = √ Rg μs + tanθ 1 - μs + tanθ
Correct Option: B
On a banked road,
Vmax² = μs + tanθ Rg 1 - μs tanθ
Maximum safe velocity of a car on the banked roadVmax = √ Rg μs + tanθ 1 - μs + tanθ