Solveeit Logo

Question

Question: The value of $v_p$ is ............................

The value of vpv_p is .........................

Answer

9.03

Explanation

Solution

This problem involves using the Work-Energy Theorem to find the final velocity of particle P.

The Work-Energy Theorem states: ΔKE=Wnet\Delta KE = W_{net} 12mvf212mui2=Wgravity+Wfriction\frac{1}{2}mv_f^2 - \frac{1}{2}mu_i^2 = W_{gravity} + W_{friction}

Given: Mass of particle P, m=2m = 2 kg Initial speed, u=10u = 10 m/s Acceleration due to gravity, g=10g = 10 m/s² Coefficient of friction, μ=0.2\mu = 0.2 Initial and final points (A and B) are at the same horizontal level, so the net work done by gravity is zero (Wgravity=0W_{gravity} = 0).

Therefore, the Work-Energy Theorem simplifies to: 12mvf212mu2=Wfriction\frac{1}{2}mv_f^2 - \frac{1}{2}mu^2 = W_{friction}

The work done by friction on an inclined plane is given by Wf=fk×LW_f = -f_k \times L, where fk=μN=μmgcosθf_k = \mu N = \mu mg \cos\theta and LL is the length of the inclined path. So, Wf=μmgcosθ×LW_f = -\mu mg \cos\theta \times L. Since Lcosθ=ΔxL \cos\theta = \Delta x (the horizontal displacement), the work done by friction on an inclined path is Wf=μmgΔxW_f = -\mu mg \Delta x. For a path composed of multiple segments, the total work done by friction is Wfriction=μmg×(total horizontal distance covered)W_{friction} = -\mu mg \times (\text{total horizontal distance covered}).

For Particle P (path ACB):

  1. Determine path dimensions:

    • Height of C from AB, hC=CE=2h_C = CE = 2 m.
    • Angle of incline for AC, θAC=30\theta_{AC} = 30^\circ.
    • Angle of incline for CB, θCB=60\theta_{CB} = 60^\circ.
    • Horizontal projection of AC: AE=CE/tan(30)=2/(1/3)=23AE = CE / \tan(30^\circ) = 2 / (1/\sqrt{3}) = 2\sqrt{3} m.
    • Horizontal projection of CB: EB=CE/tan(60)=2/3EB = CE / \tan(60^\circ) = 2 / \sqrt{3} m.
    • Total horizontal distance covered by P = AE+EB=23+2/3=(6+2)/3=8/3AE + EB = 2\sqrt{3} + 2/\sqrt{3} = (6+2)/\sqrt{3} = 8/\sqrt{3} m.
  2. Calculate work done by friction: Wfriction,P=μmg×(total horizontal distance)W_{friction,P} = -\mu mg \times (\text{total horizontal distance}) Wfriction,P=0.2×2×10×(8/3)W_{friction,P} = -0.2 \times 2 \times 10 \times (8/\sqrt{3}) Wfriction,P=4×(8/3)=32/3W_{friction,P} = -4 \times (8/\sqrt{3}) = -32/\sqrt{3} J.

  3. Apply Work-Energy Theorem: 12mvP212mu2=Wfriction,P\frac{1}{2}mv_P^2 - \frac{1}{2}mu^2 = W_{friction,P} 12(2)vP212(2)(10)2=32/3\frac{1}{2}(2)v_P^2 - \frac{1}{2}(2)(10)^2 = -32/\sqrt{3} vP2100=32/3v_P^2 - 100 = -32/\sqrt{3} vP2=10032/3v_P^2 = 100 - 32/\sqrt{3} vP2=10018.475v_P^2 = 100 - 18.475 vP2=81.525v_P^2 = 81.525 vP=81.5259.029v_P = \sqrt{81.525} \approx 9.029 m/s.

Therefore, the value of vPv_P is approximately 9.03 m/s.