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Given: mass m = 12 kg, angle of inclination theta = 30^, coefficient of friction mu = (2)/(3), and g = 10 ms⁻².

Physics

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2 parts
a

(403−60) N(40\sqrt{3} - 60) \text{ N}

b

(60+403) N(60 + 40\sqrt{3}) \text{ N}

Step-by-step solution

2 steps

Step 1: Calculate the weight of the body and its components parallel and perpendicular to the inclined plane.
Given: mass m=12 kgm = 12 \text{ kg}, angle of inclination θ=30∘\theta = 30^\circ, coefficient of friction μ=23\mu = \frac{2}{3}, and g=10 ms−2g = 10 \text{ ms}^{-2}.

The weight of the body is W=mgW = mg.

W=12 kg×10 ms−2=120 NW = 12 \text{ kg} \times 10 \text{ ms}^{-2} = 120 \text{ N}

The component of weight parallel to the plane (acting down the plane) is W∥W_{\parallel}.

W∥=Wsin⁡θ=120sin⁡30∘=120×12=60 NW_{\parallel} = W \sin\theta = 120 \sin 30^\circ = 120 \times \frac{1}{2} = 60 \text{ N}

The component of weight perpendicular to the plane is W⊥W_{\perp}.

W⊥=Wcos⁡θ=120cos⁡30∘=120×32=603 NW_{\perp} = W \cos\theta = 120 \cos 30^\circ = 120 \times \frac{\sqrt{3}}{2} = 60\sqrt{3} \text{ N}

The normal reaction force RR is equal to W⊥W_{\perp}.

R=603 NR = 60\sqrt{3} \text{ N}

The maximum static frictional force FfF_f is μR\mu R.

Ff=23×603=403 NF_f = \frac{2}{3} \times 60\sqrt{3} = 40\sqrt{3} \text{ N}

Note that W∥=60 NW_{\parallel} = 60 \text{ N} and Ff=403 N≈40×1.732=69.28 NF_f = 40\sqrt{3} \text{ N} \approx 40 \times 1.732 = 69.28 \text{ N}. Since W∥<FfW_{\parallel} < F_f, the body will not slide down the plane on its own.

Part a· 1 step

Find the value of PP if the body is at the point of moving down the plane.

  1. Determine the direction of PP and set up the force balance equation for impending downward motion.

    Since the body would not slide down on its own (W∥<FfW_{\parallel} < F_f), the external force PP must be acting down the plane to initiate motion.
    At the point of impending motion down the plane, the forces acting down the plane are balanced by the forces acting up the plane. Friction acts up the plane, opposing the downward motion.

    P+W∥=FfP + W_{\parallel} = F_f

    Substitute the calculated values:

    P+60 N=403 NP + 60 \text{ N} = 40\sqrt{3} \text{ N}

    Solve for PP:

    P=(403−60) NP = (40\sqrt{3} - 60) \text{ N}

    The value of PP is (403−60) N\boxed{(40\sqrt{3} - 60) \text{ N}}.

Part b

(60+403) N(60 + 40\sqrt{3}) \text{ N}

Find the value of PP if the body is at the point of moving up the plane.

  1. Determine the direction of PP and set up the force balance equation for impending upward motion.

    For the body to move up the plane, the external force PP must be acting up the plane.
    At the point of impending motion up the plane, the forces acting up the plane are balanced by the forces acting down the plane. Friction acts down the plane, opposing the upward motion.

    P=W∥+FfP = W_{\parallel} + F_f

    Substitute the calculated values:

    P=60 N+403 NP = 60 \text{ N} + 40\sqrt{3} \text{ N} P=(60+403) NP = (60 + 40\sqrt{3}) \text{ N}

    The value of PP is (60+403) N\boxed{(60 + 40\sqrt{3}) \text{ N}}.

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