Math Problem Statement

A child is trying to pull a sled with mass 1.65 kg by a rope. He is able to pull with tension 12.3 Newtons. Because of the friction between the ground and the sled, with a coefficient of static friction μs​=1 (unrealistic), he needs to pull the rope off the ground at some minimum angle θ to get the sled to move. Find sin⁡θ

Solution

To solve this problem, we need to find the minimum angle θ\theta at which the child needs to pull the sled to overcome static friction. We are given the following:

  • Mass of the sled, m=1.65kgm = 1.65 \, \text{kg}
  • Tension in the rope, T=12.3NT = 12.3 \, \text{N}
  • Coefficient of static friction, μs=1\mu_s = 1

Step 1: Forces Acting on the Sled

When the child pulls the sled, two major forces affect its movement:

  1. Gravitational Force: The weight of the sled is W=mgW = mg, where g=9.8m/s2g = 9.8 \, \text{m/s}^2.

    So, W=1.65kg×9.8m/s2=16.17NW = 1.65 \, \text{kg} \times 9.8 \, \text{m/s}^2 = 16.17 \, \text{N}

  2. Static Friction Force: The maximum static friction force is Ffriction=μsNF_{\text{friction}} = \mu_s N, where NN is the normal force.

Step 2: Components of the Tension Force

The tension force TT is applied at an angle θ\theta, so it has two components:

  • Horizontal Component: Tx=TcosθT_x = T \cos \theta
  • Vertical Component: Ty=TsinθT_y = T \sin \theta

Step 3: Normal Force

The normal force NN is the force exerted by the ground on the sled. It's affected by both the weight of the sled and the vertical component of the tension force: N=WTy=WTsinθN = W - T_y = W - T \sin \theta Substitute the values: N=16.17N12.3sinθN = 16.17 \, \text{N} - 12.3 \sin \theta

Step 4: Condition for Overcoming Static Friction

For the sled to start moving, the horizontal component of the tension force TxT_x must be equal to the maximum static friction force FfrictionF_{\text{friction}}: Tx=Ffriction=μsNT_x = F_{\text{friction}} = \mu_s N Substitute Tx=TcosθT_x = T \cos \theta and Ffriction=μsNF_{\text{friction}} = \mu_s N: Tcosθ=μs(WTsinθ)T \cos \theta = \mu_s (W - T \sin \theta) Since μs=1\mu_s = 1, this simplifies to: Tcosθ=WTsinθT \cos \theta = W - T \sin \theta

Step 5: Solve for sinθ\sin \theta

Now we solve the equation Tcosθ=WTsinθT \cos \theta = W - T \sin \theta. First, rearrange it as: Tcosθ+Tsinθ=WT \cos \theta + T \sin \theta = W Factor out TT: T(cosθ+sinθ)=WT (\cos \theta + \sin \theta) = W Solve for cosθ+sinθ\cos \theta + \sin \theta: cosθ+sinθ=WT=16.1712.31.315\cos \theta + \sin \theta = \frac{W}{T} = \frac{16.17}{12.3} \approx 1.315 Now, we use the identity sinθ+cosθ=2sin(θ+π4)\sin \theta + \cos \theta = \sqrt{2} \sin \left( \theta + \frac{\pi}{4} \right) to relate this expression, but since the angle requires finding components, we will work to numerically simplify.

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Math Problem Analysis

Mathematical Concepts

Trigonometry
Forces in Physics
Statics
Friction

Formulas

W = mg (Weight = mass × gravitational acceleration)
F_friction = μs × N (Static friction force)
T_x = T × cosθ (Horizontal component of tension)
T_y = T × sinθ (Vertical component of tension)
N = W - T_y (Normal force)
T × cosθ = μs(W - T × sinθ)

Theorems

Newton's Laws of Motion

Suitable Grade Level

High School (Grades 10-12)