Math Problem Statement

A javelin thrower standing at rest holds the center of the javelin behind her head, then accelerates it through a distance of 70 cm as she throws. She releases the 600 g javelin 2.0 m above the ground traveling at an angle of 30∘ above the horizontal. Top-rated javelin throwers do throw at about a 30∘ angle, not the 45∘ you might have expected, because the biomechanics of the arm allow them to throw the javelin much faster at 30∘ than they would be able to at 45∘ . In this throw, the javelin hits the ground 50 m away. Part A What was the acceleration of the javelin during the throw? Assume that it has a constant acceleration.

Solution

To find the acceleration of the javelin during the throw, we will use kinematic equations. We know that the thrower accelerated the javelin through a distance of 70cm=0.70m70 \, \text{cm} = 0.70 \, \text{m} before release. Given the final speed (vv) at release, we will first find that speed using projectile motion equations, and then use it to determine acceleration.

Step 1: Determine the initial velocity of the javelin at release.

  1. Horizontal motion:

    The horizontal distance covered is 50m50 \, \text{m}.

    The horizontal component of the velocity at release is: vx=vcosθv_x = v \cos \theta

    The time of flight (tt) is given by: t=horizontal distancevx=50vcos30t = \frac{\text{horizontal distance}}{v_x} = \frac{50}{v \cos 30^\circ}

  2. Vertical motion:

    Using the vertical displacement equation (upward is positive): y=vyt12gt2y = v_y t - \frac{1}{2} g t^2 Here, y=2my = -2 \, \text{m} (since the javelin falls 2 m from the release point), vy=vsin30v_y = v \sin 30^\circ, and g=9.8m/s2g = 9.8 \, \text{m/s}^2.

    Substituting t=50vcos30t = \frac{50}{v \cos 30^\circ}: 2=vsin30(50vcos30)129.8(50vcos30)2-2 = v \sin 30^\circ \left(\frac{50}{v \cos 30^\circ}\right) - \frac{1}{2} \cdot 9.8 \left(\frac{50}{v \cos 30^\circ}\right)^2

    Solving this equation will give us the value of vv.

Step 2: Find the acceleration using the kinematic equation.

After finding vv, we use the kinematic equation: v2=u2+2asv^2 = u^2 + 2a s where:

  • u=0u = 0 (initial velocity, as the javelin starts from rest),
  • vv = final velocity at release,
  • s=0.70ms = 0.70 \, \text{m} (distance over which acceleration occurs),
  • aa = acceleration (unknown).

Rearranging for acceleration: a=v22sa = \frac{v^2}{2s}

Let's perform the calculations to find vv and then aa.The negative value for the release velocity indicates a direction issue in our initial assumption, but we'll focus on the magnitude:

  1. Release Velocity (vv): The magnitude is approximately 23.0m/s23.0 \, \text{m/s}.

  2. Acceleration (aa): The calculated acceleration is approximately 378m/s2378 \, \text{m/s}^2.

This large value of acceleration is due to the javelin being accelerated over a short distance of 0.70 meters.

Would you like more details or have any questions about this? Here are some related questions:

  1. How does changing the release angle affect the distance the javelin travels?
  2. What is the maximum height reached by the javelin during its flight?
  3. How much time does the javelin spend ascending and descending?
  4. How would a different acceleration distance affect the release speed?
  5. What is the role of initial speed in determining the range of projectile motion?

Tip: Always check the sign convention in projectile motion problems to avoid confusion with velocity directions.

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Math Problem Analysis

Mathematical Concepts

Projectile Motion
Kinematics
Trigonometry

Formulas

Horizontal component: v_x = v * cos(θ)
Vertical displacement: y = v_y * t - (1/2) * g * t^2
Kinematic equation: v^2 = u^2 + 2a * s

Theorems

Projectile motion equations
Kinematic equations

Suitable Grade Level

Grades 11-12 or early college physics