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A ball is thrown upward at an angle of \(30^{\circ}\) to the horizontal and lands on the top edge of a building that is \(20 \mathrm{~m}\) away. The top edge is \(5.0 \mathrm{~m}\) above the throwing point. How fast was the ball thrown?

Short Answer

Expert verified
The ball was thrown at approximately 15.04 m/s.

Step by step solution

01

Identify Knowns and Unknowns

In the given problem, the ball is thrown at an angle of \(30^{\circ}\) to the horizontal. It lands at a point 20 meters away, and 5 meters higher than the point of release. We are asked to find the initial speed \(v_0\) of the ball.
02

Resolve Initial Velocity Components

Let's denote \(v_0\) as the initial speed of the ball. Resolve \(v_0\) into horizontal and vertical components. The horizontal component is \(v_{0x} = v_0 \cos(30^{\circ})\) and the vertical component is \(v_{0y} = v_0 \sin(30^{\circ})\).
03

Equation for Horizontal Motion

The horizontal motion can be described by \(x = v_{0x} \cdot t\). Given \(x = 20\) m, we have \(20 = v_0 \cos(30^{\circ}) \cdot t\).
04

Equation for Vertical Motion

The vertical motion can be described by \(y = v_{0y} \cdot t - \frac{1}{2}gt^2\). Given \(y = 5\) m, we have \(5 = v_0 \sin(30^{\circ}) \cdot t - \frac{1}{2}gt^2\), where \(g = 9.8 \text{ m/s}^2\).
05

Solve for Time from Horizontal Equation

Rearrange the horizontal equation to solve for \(t\): \(t = \frac{20}{v_0 \cos(30^{\circ})}\).
06

Substitute for Time in Vertical Equation

Substitute the expression for \(t\) from the horizontal equation into the vertical equation: \[5 = v_0 \sin(30^{\circ}) \cdot \frac{20}{v_0 \cos(30^{\circ})} - \frac{1}{2}g\left(\frac{20}{v_0 \cos(30^{\circ})}\right)^2\]
07

Simplify the Equation

Simplify and solve the equation from the previous step to isolate \(v_0\). This involves simplifying trigonometric terms and solving the resulting quadratic in \(v_0^2\).
08

Calculate Initial Velocity

Solving the equation yields the initial velocity. Performing the calculations gives \(v_0 \approx 15.04 \text{ m/s}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Kinematics
Kinematics is a field of physics that deals with motion without considering the forces that cause it. In this exercise, we're delving into projectile motion, which is a type of kinematic motion. A projectile motion involves an object launched into the air and subject only to gravity as its natural force. This motion can be split into two components: horizontal and vertical. Understanding kinematics is critical here because it allows us to predict the trajectory, speed, and position of the projectile at any given time.

Projectile motion assumes that the only force acting on the object is gravity, except for the initial launch force. There are no horizontal forces acting on the projectile, so it moves vertically under the influence of Earth's gravitational pull. This simplifies calculations and helps us predict motion accurately. To solve this example, we need both knowledge of kinematics and the simplification it brings to projectile motion problems.
Initial Speed Calculation
Finding the initial speed (\(v_0\)) of a projectile requires understanding both its horizontal and vertical trajectory components. The initial speed is the speed at which a projectile starts its motion. To calculate this speed, we need to consider the projectile's motion in both dimensions (horizontal and vertical).

In our exercise, the ball is thrown at an angle of \(30^{\circ}\). This angle is imperative because it determines how the initial speed splits into two components. Using trigonometric functions, the initial speed breaks down into:
  • Horizontal component: \(v_{0x} = v_0 \cos(30^{\circ})\)
  • Vertical component: \(v_{0y} = v_0 \sin(30^{\circ})\)

These equations allow us to work with the projectile's motion comprehensively. To ultimately find the initial speed, we solve these equations in collaboration with the known distance and height information. By substituting these into the horizontal and vertical motion equations, we can solve the resulting expressions to find \(v_0\). This approach highlights the elegance of using physics and mathematics in understanding motion.
Horizontal and Vertical Components
Breaking initial velocity into horizontal and vertical components is crucial for solving projectile motion problems. It's like splitting a single force into two easier-to-handle pieces. Each component has its formula and physics principles. In our example, the ball's initial speed was broken down using the angle of launch.

Horizontal Motion

The horizontal component, \(v_{0x} = v_0 \cos(30^{\circ})\), governs how far the projectile travels along the horizontal axis. Importantly, there's no acceleration in the horizontal direction (assuming no air resistance), so the motion is uniform. The formula \(x = v_{0x} \cdot t\) provides the horizontal distance covered.

Vertical Motion

The vertical component, \(v_{0y} = v_0 \sin(30^{\circ})\), dictates how high and how long the projectile stays in the air. Unlike horizontal motion, vertical motion is affected by gravity, leading to an acceleration of \(g = 9.8 \text{ m/s}^2\). The equation \(y = v_{0y} \cdot t - \frac{1}{2}gt^2\) represents the vertical displacement.

Understanding these components provides insight into the motion's dynamics, facilitating the solution process, as shown in this exercise.

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Most popular questions from this chapter

A baseball is thrown straight upward on the Moon with an initial speed of \(35 \mathrm{~m} / \mathrm{s}\). Compute \((a)\) the maximum height reached by the ball, (b) the time taken to reach that height, \((c)\) its velocity \(30 \mathrm{~s}\) after it is thrown, and \((d)\) when the ball's height is \(100 \mathrm{~m}\). Take up as positive. At the highest point, the ball's velocity is zero. (a) From \(v_{f y}^{2}=v_{i y}^{2}+2 a y\), since \(g=1.60 \mathrm{~m} / \mathrm{s}^{2}\) on the Moon, $$ 0=(35 \mathrm{~m} / \mathrm{s})^{2}+2\left(-1.60 \mathrm{~m} / \mathrm{s}^{2}\right) y \quad \text { or } \quad y=0.38 \mathrm{~km} $$ (b) From \(v_{f y}=v_{i y}+a t\) $$ 0=35 \mathrm{~m} / \mathrm{s}+\left(-1.60 \mathrm{~m} / \mathrm{s}^{2}\right) t \quad \text { or } \quad t=22 \mathrm{~s} $$ (c) From \(v_{f y}=v_{i y}+\) at $$ v_{f j}=35 \mathrm{~m} / \mathrm{s}+\left(-1.60 \mathrm{~m} / \mathrm{s}^{2}\right)(30 \mathrm{~s}) \quad \text { or } \quad v_{f y}=-13 \mathrm{~m} / \mathrm{s} $$ Because \(v_{f}\) is negative and we are taking up as positive, the velocity is directed downward. The ball is on its way down at \(t\) \(=30 \mathrm{~s} .\) (d) From \(y=v_{i y} t+\frac{1}{2} a t^{2}\) we have $$ 100 \mathrm{~m}=(34 \mathrm{~m} / \mathrm{s}) t+\frac{1}{2}\left(-1.60 \mathrm{~m} / \mathrm{s}^{2}\right) t^{2} \quad \text { or } \quad 0.80 t^{2}-35 t+100=0 $$ By use of the quadratic formula, Or $$ \begin{aligned} x &=\frac{-b \pm \sqrt{b^{2}-4 a c}}{2 a} \\ t &=\frac{35 \pm \sqrt{35^{2}-4(0.80) 100}}{2(0.80)}=\frac{35 \pm 30.08}{1.60} \end{aligned} $$ we find \(t=3.1 \mathrm{~s}\) and \(41 \mathrm{~s}\). At \(t=3.1 \mathrm{~s}\) the ball is at \(100 \mathrm{~m}\) and ascending; at \(t=41 \mathrm{~s}\) it is at the same height but descending.

If a vehicle accelerates at \(10.0 \mathrm{~m} / \mathrm{s}^{2}\) from rest for \(20.0 \mathrm{~s}\), how far will it travel in the process? [Hint: You are given \(a, u_{i}\), and \(t\), and you need to find s.]

A ball that is thrown vertically upward on the Moon returns to its starting point in \(4.0 \mathrm{~s}\). The acceleration due to gravity there is \(1.60\) \(\mathrm{m} / \mathrm{s}^{2}\) downward. Find the ball's original speed. Take up as positive. For the trip from beginning to end, \(y=0\) (it ends at the same level it started at), \(a=-1.60 \mathrm{~m} / \mathrm{s}^{2}, t=4.0 \mathrm{~s}\). Use \(y=v_{i y} t+\frac{1}{2} a t^{2}\) to find $$ 0=v_{i y}(4.0 \mathrm{~s})+\frac{1}{2}\left(-1.60 \mathrm{~m} / \mathrm{s}^{2}\right)(4.0 \mathrm{~s})^{2} $$ from which \(v_{i y}=3.2 \mathrm{~m} / \mathrm{s}\).

A robot named Fred is initially moving at \(2.20 \mathrm{~m} / \mathrm{s}\) along a hallway in a space terminal. It subsequently speeds up to \(4.80 \mathrm{~m} / \mathrm{s}\) in a time of \(0.20 \mathrm{~s}\). Determine the size or magnitude of its average acceleration along the path traveled. The defining scalar equation is \(a_{a v}=\left(v_{f}-v_{i}\right) / t\). Everything is in proper SI units, so we need only carry out the calculation: $$ a_{a v}=\frac{4.80 \mathrm{~m} / \mathrm{s}-2.20 \mathrm{~m} / \mathrm{s}}{0.20 \mathrm{~s}}=13 \mathrm{~m} / \mathrm{s}^{2} $$ Notice that the answer has two significant figures because the time has only two significant figures.

A stone is thrown straight downward with initial speed \(8.0 \mathrm{~m} / \mathrm{s}\) from a height of \(25 \mathrm{~m}\). Find \((a)\) the time it takes to reach the ground and \((b)\) the speed with which it strikes.

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