/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 40 A grasshopper hops down a level ... [FREE SOLUTION] | 91Ó°ÊÓ

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A grasshopper hops down a level road. On each hop, the grasshopper launches itself at angle \(\theta_{0}=45^{\circ}\) and achieves a range \(R=1.0 \mathrm{~m}\). What is the average horizontal speed of the grasshopper as it progresses down the road? Assume that the time spent on the ground between hops is negligible.

Short Answer

Expert verified
The average horizontal speed is approximately 2.21 m/s.

Step by step solution

01

Understanding the Relationship

The range of a projectile is given by the formula \( R = \frac{v_0^2 \sin(2\theta_0)}{g} \), where \( v_0 \) is the initial velocity, \( \theta_0 \) is the launch angle, and \( g \) is the acceleration due to gravity (approximately \( 9.8 \, \text{m/s}^2 \)). Since \( R = 1.0 \, \text{m} \) and \( \theta_0 = 45^{\circ} \), we know that \( \sin(90^{\circ}) = 1 \). Thus the formula simplifies to \( R = \frac{v_0^2}{g} \).
02

Solving for the Initial Velocity

Rearrange the simplified range equation to solve for \( v_0 \): \( v_0^2 = R \cdot g \). Substituting the given range and the value of \( g \), we find \( v_0^2 = 1.0 \cdot 9.8 \). Therefore, \( v_0 = \sqrt{9.8} \approx 3.13 \, \text{m/s} \).
03

Calculating the Horizontal Speed

The horizontal component of the velocity is \( v_{x} = v_0 \cos(\theta_0) \). Since \( \theta_0 = 45^{\circ} \), \( \cos(45^{\circ}) = \frac{1}{\sqrt{2}} \approx 0.707 \). Therefore, \( v_{x} = 3.13 \cdot 0.707 \) which results in \( v_{x} \approx 2.21 \, \text{m/s} \).
04

Finalizing the Average Speed

Since the problem states the time on the ground between hops is negligible, the average horizontal speed is essentially the calculated horizontal component of the velocity. Thus, the average horizontal speed of the grasshopper as it hops down the road is \( v_{x} \approx 2.21 \, \text{m/s} \).

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Key Concepts

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

Initial Velocity
Initial velocity is the speed at which an object is launched into the air. It combines both the horizontal and vertical components of motion. When discussing projectile motion like a grasshopper's hop, understanding initial velocity is essential.
For instance, in our grasshopper problem, the range equation is used to find the initial velocity. The range equation is:
  • \( R = \frac{v_0^2 \sin(2\theta_0)}{g} \)
This relates the range \( R \), initial velocity \( v_0 \), launch angle \( \theta_0 \), and gravitational acceleration \( g \). When solving for initial velocity, especially with a known angle of 45 degrees, this equation simplifies considerably. This simplification happens because \( \sin(90^\circ) = 1 \).
From the solution, we rearranged the equation to \( v_0^2 = R \cdot g \) and solved for \( v_0 \). As we calculated, \( v_0 \approx 3.13 \text{ m/s} \). This initial velocity helps us break down further components of motion.
Horizontal Speed
Horizontal speed is the constant speed at which an object moves along the horizontal axis. Once an object is launched and no other forces act on it (except gravity), this speed remains constant.
In the grasshopper scenario, horizontal speed \( v_x \) is derived from the initial velocity and the launch angle. The equation used is:
  • \( v_x = v_0 \cos(\theta_0) \)
Since a 45-degree launch angle was provided, the calculation becomes easier using \( \cos(45^\circ) = \frac{1}{\sqrt{2}} \), which is approximately 0.707. Plugging in the initial velocity \( v_0 \approx 3.13 \text{ m/s} \) from previous calculations, we determine that \( v_x \approx 2.21 \text{ m/s} \).
This horizontal speed is crucial for solving many projectile problems and understanding the motion over a horizontal plane.
Launch Angle
Launch angle significantly affects the range and trajectory of a projectile. It is the angle at which an object is launched relative to the horizontal plane.
In our example, the grasshopper launches at an angle \( \theta_0 = 45^\circ \). This specific angle often maximizes the range in projectile motion scenarios when considering identical start and end heights. The reason is that at this angle, both the horizontal and vertical components of the initial velocity have equal magnitudes. This balance results in optimal range.
In calculations, angles different from 45 degrees would yield different maximum heights and ranges. Launch angle is fundamental in determining how far an object can travel horizontally. Understanding its role is vital for predicting projectile paths accurately.

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Most popular questions from this chapter

A batter hits a fly ball which leaves the bat \(0.90 \mathrm{~m}\) above the ground at an angle of \(61^{\circ}\) with an initial speed of \(28 \mathrm{~m} / \mathrm{s}\) heading toward centerfield. Ignore air resistance. \((a)\) How far from home plate would the ball land if not caught? \((b)\) The ball is caught by the centerfielder who, starting at a distance of \(105 \mathrm{~m}\) from home plate, runs straight toward home plate at a constant speed and makes the catch at ground level. Find his speed.

(II) At what projection angle will the range of a projectile cqual its maximum height?

Graphically determine the resultant of the following three vector displacements: (1) \(24 \mathrm{~m}, 36^{\circ}\) north of east; (2) \(18 \mathrm{~m}\) \(37^{\circ}\) east of north; and (3) \(26 \mathrm{~m}, 33^{\circ}\) west of south.

\(\overrightarrow{\mathbf{V}}\) is a vector 24.8 units in magnitude and points at an angle of \(23.4^{\circ}\) above the negative \(x\) axis. \((a)\) Sketch this vector. (b) Calculate \(V_{x}\) and \(V_{y} \cdot(c)\) Use \(V_{x}\) and \(V_{y}\) to obtain (again) the magnitude and direction of \(\overrightarrow{\mathbf{V}}\). [Note: Part \((c)\) is a good way to check if you've resolved your vector correctly.]

A particle has a velocity of \(\vec{\mathbf{v}}=(-2.0 \hat{\mathbf{i}}+3.5 t \mathbf{j}) \mathrm{m} / \mathrm{s}\) . The particle starts at \(\vec{\mathbf{r}}=(1.5 \hat{\mathrm{i}}-3.1 \hat{\mathrm{j}}) \mathrm{m}\) at \(t=0 .\) Give the position and acceleration as a function of time. What is the shape of the resulting path?

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