Solveeit Logo

Question

Question: Two blocks of mass "2kg" & "3kg" respectively are placed on rough inclined having inclination angle ...

Two blocks of mass "2kg" & "3kg" respectively are placed on rough inclined having inclination angle θ\theta = 37° as shown in the diagram (N is the normal reaction between the two blocks):-

A

If μ₁ = μ2 = 0.5 ; a₁ = a2 ≠ 0, N = 0

B

If μ₁ = μ₂ = 0.5 ; a₁ = a2 ≠ 0, N≠0

C

If μ₁ = 0.6, μ2 = 0.1 ; a₁ = a2 = 3.6 m/s², N≠0

D

If μ₁ = 0.1, μ2 = 0.6 ; a₁ > a2, N = 0

Answer

If μ₁ = μ2 = 0.5 ; a₁ = a2 ≠ 0, N = 0, If μ₁ = 0.6, μ2 = 0.1 ; a₁ = a2 = 3.6 m/s², N≠0, If μ₁ = 0.1, μ2 = 0.6 ; a₁ > a2, N = 0

Explanation

Solution

To analyze the motion of the two blocks, we first calculate the acceleration each block would have if it were moving independently down the incline. The acceleration of a block of mass mm with coefficient of kinetic friction μ\mu on an incline of angle θ\theta is given by:

aind=gsinθμgcosθa_{ind} = g \sin\theta - \mu g \cos\theta

Given: m1=2 kgm_1 = 2 \text{ kg}, m2=3 kgm_2 = 3 \text{ kg} θ=37\theta = 37^\circ We use g=10 m/s2g = 10 \text{ m/s}^2. sin(37)0.6\sin(37^\circ) \approx 0.6 cos(37)0.8\cos(37^\circ) \approx 0.8

So, gsinθ=10×0.6=6 m/s2g \sin\theta = 10 \times 0.6 = 6 \text{ m/s}^2. And gcosθ=10×0.8=8 m/s2g \cos\theta = 10 \times 0.8 = 8 \text{ m/s}^2.

Thus, aind=68μa_{ind} = 6 - 8\mu.

Now, let's analyze each option:

Option 1: If μ1=μ2=0.5\mu_1 = \mu_2 = 0.5; a1=a20a_1 = a_2 \neq 0, N=0N = 0

Calculate independent accelerations: a1ind=68(0.5)=64=2 m/s2a_1^{ind} = 6 - 8(0.5) = 6 - 4 = 2 \text{ m/s}^2 a2ind=68(0.5)=64=2 m/s2a_2^{ind} = 6 - 8(0.5) = 6 - 4 = 2 \text{ m/s}^2

Since a1ind=a2inda_1^{ind} = a_2^{ind}, both blocks tend to move with the same acceleration. Therefore, they will move together with a1=a2=2 m/s2a_1 = a_2 = 2 \text{ m/s}^2. As there is no relative motion tendency, there will be no normal force between them, so N=0N=0. The conditions a1=a20a_1 = a_2 \neq 0 and N=0N = 0 are met. This option is correct.

Option 2: If μ1=μ2=0.5\mu_1 = \mu_2 = 0.5; a1=a20a_1 = a_2 \neq 0, N0N \neq 0

From the analysis of Option 1, when μ1=μ2=0.5\mu_1 = \mu_2 = 0.5, we found that N=0N=0. This option states N0N \neq 0, which contradicts our finding. This option is incorrect.

Option 3: If μ1=0.6,μ2=0.1\mu_1 = 0.6, \mu_2 = 0.1; a1=a2=3.6 m/s2a_1 = a_2 = 3.6 \text{ m/s}^2, N0N \neq 0

Calculate independent accelerations: a1ind=68(0.6)=64.8=1.2 m/s2a_1^{ind} = 6 - 8(0.6) = 6 - 4.8 = 1.2 \text{ m/s}^2 a2ind=68(0.1)=60.8=5.2 m/s2a_2^{ind} = 6 - 8(0.1) = 6 - 0.8 = 5.2 \text{ m/s}^2

Since a2ind>a1inda_2^{ind} > a_1^{ind}, block 2 (the one behind) tends to accelerate faster than block 1 (the one in front). This means block 2 will push block 1, so they will move together with a common acceleration aa, and N0N \neq 0. To find the common acceleration aa, treat the two blocks as a single system with total mass M=m1+m2=2+3=5 kgM = m_1 + m_2 = 2 + 3 = 5 \text{ kg}. The net force down the incline on the combined system is: Fnet=(m1+m2)gsinθ(μ1m1gcosθ+μ2m2gcosθ)F_{net} = (m_1+m_2)g \sin\theta - (\mu_1 m_1 g \cos\theta + \mu_2 m_2 g \cos\theta) Fnet=(2+3)(6)(0.6×2×8+0.1×3×8)F_{net} = (2+3)(6) - (0.6 \times 2 \times 8 + 0.1 \times 3 \times 8) Fnet=5×6(9.6+2.4)F_{net} = 5 \times 6 - (9.6 + 2.4) Fnet=3012=18 NF_{net} = 30 - 12 = 18 \text{ N} The common acceleration is a=FnetM=18 N5 kg=3.6 m/s2a = \frac{F_{net}}{M} = \frac{18 \text{ N}}{5 \text{ kg}} = 3.6 \text{ m/s}^2. This matches the given acceleration a1=a2=3.6 m/s2a_1 = a_2 = 3.6 \text{ m/s}^2. Since a2ind>a1inda_2^{ind} > a_1^{ind}, there must be a normal force N0N \neq 0 for them to move together. (We can calculate NN for verification. For m1m_1: m1a=m1gsinθ+Nμ1m1gcosθm_1 a = m_1 g \sin\theta + N - \mu_1 m_1 g \cos\theta. 2×3.6=2×6+N0.6×2×82 \times 3.6 = 2 \times 6 + N - 0.6 \times 2 \times 8 7.2=12+N9.67.2 = 12 + N - 9.6 7.2=2.4+N    N=4.8 N7.2 = 2.4 + N \implies N = 4.8 \text{ N}, which is non-zero.) The conditions a1=a2=3.6 m/s2a_1 = a_2 = 3.6 \text{ m/s}^2 and N0N \neq 0 are met. This option is correct.

Option 4: If μ1=0.1,μ2=0.6\mu_1 = 0.1, \mu_2 = 0.6; a1>a2a_1 > a_2, N=0N = 0

Calculate independent accelerations: a1ind=68(0.1)=60.8=5.2 m/s2a_1^{ind} = 6 - 8(0.1) = 6 - 0.8 = 5.2 \text{ m/s}^2 a2ind=68(0.6)=64.8=1.2 m/s2a_2^{ind} = 6 - 8(0.6) = 6 - 4.8 = 1.2 \text{ m/s}^2

Since a1ind>a2inda_1^{ind} > a_2^{ind}, block 1 (the one in front) tends to accelerate faster than block 2 (the one behind). This means block 1 will move away from block 2, and they will separate. In this case, there will be no normal force between them, so N=0N=0. The accelerations will be their independent accelerations: a1=5.2 m/s2a_1 = 5.2 \text{ m/s}^2 and a2=1.2 m/s2a_2 = 1.2 \text{ m/s}^2. The conditions a1>a2a_1 > a_2 (5.2>1.25.2 > 1.2) and N=0N = 0 are met. This option is correct.

Therefore, options 1, 3, and 4 are correct.