/*! 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 35 The velocity of a \(3.00 \mathrm... [FREE SOLUTION] | 91Ó°ÊÓ

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The velocity of a \(3.00 \mathrm{~kg}\) particle is given by \(\vec{v}=\left(8.00 \hat{i}+3.00 t^{2} \hat{i}\right)\) \(\mathrm{m} / \mathrm{s}\), with time \(t\) in seconds. At the instant the net force on the particle has a magnitude of \(35.0 \mathrm{~N}\), what are the direction (relative to the positive direction of the \(x\) axis) of (a) the net force and (b) the particle's direction of travel?

Short Answer

Expert verified
(a) 90°; (b) 54°

Step by step solution

01

Understand the Velocity Equation

The given velocity of the particle is \( \vec{v}=\left(8.00 \hat{i}+3.00 t^{2} \hat{j}\right) \mathrm{m/s} \). It is time-dependent in the \( y \)-direction and constant in the \( x \)-direction.
02

Determine the Velocity Components

Identify the velocity components: \( v_x = 8.00 \) m/s and \( v_y = 3.00 t^2 \) m/s. These components describe the particle’s velocity direction in the \( x \) and \( y \) axes, respectively.
03

Calculate Acceleration Components

The acceleration is the derivative of the velocity. Compute the acceleration: \( a_x = 0 \) m/s² and \( a_y = \frac{d}{dt}(3.00t^2) = 6.00t \) m/s².
04

Use Newton's Second Law

Apply Newton's second law, \( \vec{F} = m\vec{a} \), to find the force components: \( F_x = m \cdot a_x = 0 \) N and \( F_y = m \cdot a_y = 3.00 \times 6.00t = 18.0t \) N.
05

Set Up Net Force Equation

The magnitude of the net force is given as 35.0 N. Therefore, \( \sqrt{F_x^2 + F_y^2} = 35.0 \) N. Since \( F_x = 0 \), it simplifies to \( F_y = 35.0 \) N. Solve \( 18.0t = 35.0 \) to find \( t = \frac{35.0}{18.0} \approx 1.94 \) seconds.
06

Determine Direction of Net Force

Since \( F_y = 35.0 \) N and \( F_x = 0 \), the net force is directed along the positive \( y \)-axis. The angle relative to the \( x \)-axis is \( 90^\circ \).
07

Determine Particle's Direction of Travel

At \( t = 1.94 \) seconds, compute the velocity direction: \( v_x = 8 \) m/s and \( v_y = 3.00 \cdot (1.94)^2 = 11.29 \) m/s. The angle \( \theta \) relative to the \( x \)-axis is \( \tan^{-1}\left(\frac{v_y}{v_x}\right) \), calculate \( \tan^{-1}\left(\frac{11.29}{8}\right) \approx 54.0^\circ \).

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Key Concepts

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

Velocity
Velocity is a fundamental concept in physics that describes the rate at which an object changes its position. In this problem, the velocity of the particle is given by the vector \( \vec{v}=\left(8.00 \hat{i}+3.00 t^{2} \hat{j}\right) \mathrm{m/s} \). This equation means the particle's movement can be described by two components: a constant velocity in the \( x \)-direction (8.00 m/s) and a time-dependent velocity in the \( y \)-direction (3.00 \cdot t^2) m/s.
  • The \( x \)-component of velocity, \( v_x = 8.00 \) m/s, indicates a steady motion in the horizontal direction.
  • The \( y \)-component of velocity, \( v_y = 3.00 t^2 \) m/s, shows that the particle's velocity in the vertical direction increases as time passes.
This results in a path that curves, continuously changing the direction of travel. The velocity direction and magnitude at any given time can be understood by these components. Velocity, therefore, provides essential insight into how fast and in what direction a particle is moving, which is critical for predicting the object's future position.
Force
Force, as explained through Newton's second law, represents the interaction that causes an object to accelerate. The relation shown by the law is \( \vec{F} = m \vec{a} \), where \( \vec{F} \) is force, \( m \) is mass, and \( \vec{a} \) is acceleration. In this problem, we are applying this concept to a \( 3.00 \) kg particle. Using the acceleration components from the velocity derivation:- The horizontal acceleration component \( a_x = 0 \) (derivative of constant \( 8.00 \) m/s is zero)- The vertical acceleration component \( a_y = 6.00 t \) (derivative of \( 3.00t^2 \) m/s is \( 6.00t \) m/s²)This leads to force components:
  • \( F_x = m \cdot a_x = 0 \) N
  • \( F_y = m \cdot a_y = 18.0 t \) N
Given the net force is \( 35.0 \) N and \( F_x = 0 \), we determine \( F_y = 35.0 \) N, ensuring the force is along the \( y \)-direction at this specific moment. Understanding how force components result from acceleration helps students grasp the real-life applications of Newton's second law, ensuring they see force as not merely an abstract concept but an actionable one affecting everyday physics.
Acceleration
Acceleration measures how quickly an object changes its velocity, typically as a result of an acting force. In this exercise, acceleration derives from the velocity's time-varying component. Particularly, we calculate the acceleration components by differentiating the velocity components with respect to time. The outcome is:
  • \( a_x = 0 \) m/s², since the velocity in the \( x \)-direction is constant
  • \( a_y = 6.00t \) m/s², since the velocity in the \( y \)-direction is \( 3.00t^2 \)
Acceleration is vital for understanding how objects move and interact in a physical space. It links directly to force, as described by Newton's second law. When students see that the acceleration is what dictates the varying component of force, they can better appreciate how acceleration's magnitude and direction are continually altering except when velocities are constant. Finally, by setting the calculated force equal to the given force, we found the time at which the particle's acceleration aligns with that force magnitude, closing the loop of understanding the dynamic nature of motions compelled by forces.

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Most popular questions from this chapter

A worker drags a crate across a factory floor by pulling on a rope tied to the crate. The worker exerts a force of magnitude \(F=450 \mathrm{~N}\) on the rope, which is inclined at an upward angle \(\theta=38^{\circ}\) to the horizontal, and the floor exerts a horizontal force of magnitude \(f=125 \mathrm{~N}\) that opposes the motion. Calculate the magnitude of the acceleration of the crate if (a) its mass is \(310 \mathrm{~kg}\) and \((\mathrm{b})\) its weight is \(310 \mathrm{~N}\).

There are two forces on the \(2.00 \mathrm{~kg}\) box in the overhead view of Fig. 5-31, but only one is shown. For \(F_{1}=20.0 \mathrm{~N}, a=12.0 \mathrm{~m} / \mathrm{s}^{2}\), and \(\theta=30.0^{\circ}\), find the second force (a) in unit-vector notation and as (b) a magnitude and (c) an angle relative to the positive direction of the \(x\) axis.

A shot putter launches a \(7.260 \mathrm{~kg}\) shot by pushing it along a straight line of length \(1.650 \mathrm{~m}\) and at an angle of \(34.10^{\circ}\) from the horizontal, accelerating the shot to the launch speed from its initial speed of \(2.500 \mathrm{~m} / \mathrm{s}\) (which is due to the athlete's preliminary motion). The shot leaves the hand at a height of \(2.110 \mathrm{~m}\) and at an angle of \(34.10^{\circ}\), and it lands at a horizontal distance of \(15.90 \mathrm{~m}\). What is the magnitude of the athlete's average force on the shot during the acceleration phase? (Hint: Treat the motion during the acceleration phase as though it were along a ramp at the given angle.)

Only two horizontal forces act on a \(3.0 \mathrm{~kg}\) body that can move over a frictionless floor. One force is \(9.0 \mathrm{~N}\), acting due east, and the other is \(8.0 \mathrm{~N}\), acting \(62^{\circ}\) north of west. What is the magnitude of the body's acceleration?

Two horizontal forces act on a \(2.0 \mathrm{~kg}\) chopping block that can slide over a frictionless kitchen counter, which lies in an \(x y\) plane. One force is \(\vec{F}_{1}=(3.0 \mathrm{~N}) \hat{\mathrm{i}}+(4.0 \mathrm{~N}) \hat{\mathrm{j}}\). Find the acceleration of the chopping block in unit-vector notation when the other force is (a) \(\vec{F}_{2}=(-3.0 \mathrm{~N}) \hat{\mathrm{i}}+(-4.0 \mathrm{~N}) \hat{\mathrm{j}}\) (b) \(\vec{F}_{2}=(-3.0 \mathrm{~N}) \hat{\mathrm{i}}+(4.0 \mathrm{~N}) \hat{\mathrm{j}}\) and \((\mathrm{c}) \vec{F}_{2}=(3.0 \mathrm{~N}) \hat{\mathrm{i}}+(-4.0 \mathrm{~N}) \hat{\mathrm{j}}\)

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