/*! 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 60 A particle of mass \(m\) moving ... [FREE SOLUTION] | 91Ó°ÊÓ

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A particle of mass \(m\) moving along the \(x\) -axis experiences the net force \(F_{x}=c l,\) where \(c\) is a constant. The particle has velocity \(v_{\mathrm{dr}}\) at \(t=0 .\) Find an algebraic expression for the particle's velocity \(v_{x}\) at a later time \(t\).

Short Answer

Expert verified
The velocity of the particle at time \(t\) is given by the expression: \(v_x = v_{dr} + c\cdot l \cdot t / m\)

Step by step solution

01

Apply Newton's Second Law

Start by applying Newton's Second Law which states that the force applied on an object equals its mass times its acceleration. Therefore, set up the following equation: \(F_x = m \cdot a_x\). Then, substitute the provided force \(F_x = c\cdot l\) and the definition of acceleration (\(a_x = dv_x / dt\)) into the equation. This yields the differential equation: \(c\cdot l = m dv_x/dt\)
02

Integrate the Differential Equation

Rearranging the terms, we get \(dv_x = c \cdot l \cdot dt / m\). Now, integrate both sides from \(0\) to \(t\) for dt, and from \(v_{dr}\) to \(v_x\) for \(dv_x\). This gives you \(\int_{v_{dr}}^{v_x} dv_x = \int_{0}^{t} (c\cdot l \cdot dt) / m\)
03

Evaluate the Integrals

Evaluating the integrals gives: \(v_x - v_{dr} = c\cdot l \cdot t / m\)
04

Solve for \(v_x\)

Finally, solve for \(v_x\) to get the velocity of the particle at time \(t\). This gives: \(v_x = v_{dr} + c\cdot l \cdot t / m\).

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Key Concepts

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

Differential Equations
Differential equations play a vital role in understanding physical systems. They describe relationships between functions and their derivatives, which often reflect how a system changes over time. In the context of Newton's Second Law, these equations express the relationship between force, mass, and acceleration, such as in our exercise where we have the equation: \( F_x = m \cdot a_x \).
This particular exercise introduces a differential equation by substituting acceleration with its mathematical form using velocity: \( a_x = \frac{dv_x}{dt} \). This transforms our understanding of force into a function of change in velocity over time. Our differential equation becomes \( c \cdot l = m \frac{dv_x}{dt} \).
Understanding differential equations helps in predicting future states of systems by solving how variables change over time. This is crucial in physics as it allows us to determine the velocity of particles or objects when subjected to certain forces.
Integration
Integration is an essential mathematical tool to solve differential equations, especially in physics to find cumulative effects. In our problem, after deriving the differential equation \( c \cdot l = m \frac{dv_x}{dt} \), we rearrange to \( dv_x = \frac{c \cdot l}{m} \cdot dt \).
Integration comes into play to determine the velocity \( v_x \) at a time \( t \). By integrating both sides, we accumulate the change in velocity from its initial value \( v_{dr} \) to \( v_x \):
  • \( \int_{v_{dr}}^{v_x} dv_x \)
  • \( \int_{0}^{t} \frac{c \cdot l}{m} \cdot dt \)
This process results in \( v_x - v_{dr} = \frac{c \cdot l \cdot t}{m} \).
Integration thus helps us find explicit expressions for variables and understand how cumulative changes lead to a system's evolution over time.
Acceleration
Acceleration is a key concept in dynamics, typically defined as the rate of change of velocity with respect to time \( a_x = \frac{dv_x}{dt} \). Through Newton's Second Law, it relates directly to the forces acting upon an object.
In this exercise, the constant force \( F_x = c \cdot l \) leads to a constant acceleration \( \frac{c \cdot l}{m} \). This shows how a steady force results in a uniform acceleration. Understanding this allows us to calculate how velocity changes over time. The resulting velocity is a sum of the initial velocity and this constant incremental change due to the force. By knowing this, we compute how the velocity \( v_x \) increases linearly over time from the initial \( v_{dr} \) when a constant force is applied.
This highlights the importance of acceleration in determining motion and predicting an object's future position and velocity.

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