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How large a force is required to accelerate a \(1300-\mathrm{kg}\) car from rest to a speed of \(20 \mathrm{~m} / \mathrm{s}\) in a horizontal distance of \(80 \mathrm{~m}\) ?

Short Answer

Expert verified
A force of 3250 N is required.

Step by step solution

01

Identify the known variables

We are given the mass of the car, \( m = 1300 \text{ kg} \), the final velocity \( v = 20 \text{ m/s} \), and the displacement \( d = 80 \text{ m} \). The initial velocity \( u = 0 \text{ m/s}\) since the car starts from rest.
02

Use the kinematic equation to find acceleration

Use the kinematic equation \( v^2 = u^2 + 2ad \) to find the acceleration \( a \). Substitute the known values into the equation:\[ (20)^2 = 0^2 + 2a \times 80 \]This simplifies to:\[ 400 = 160a \]Solve for \( a \):\[ a = \frac{400}{160} = 2.5 \text{ m/s}^2 \]
03

Calculate the force using Newton's second law

Use Newton's second law \( F = ma \) to calculate the force. Now that you have \( a = 2.5 \text{ m/s}^2 \) and \( m = 1300 \text{ kg} \), substitute these values into the equation:\[ F = 1300 \times 2.5 = 3250 \text{ N} \]

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Key Concepts

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

Kinematic Equations
In physics, kinematic equations are essential for solving problems related to motion. These equations describe how objects move in terms of position, velocity, and acceleration over time. They are particularly useful in scenarios where acceleration is constant. One of the fundamental kinematic equations used in this problem is:
  • The equation: \( v^2 = u^2 + 2ad \) helps us find the acceleration needed when distance is known.
  • Here, \( v \) is the final velocity, \( u \) is the initial velocity, \( a \) is the acceleration, and \( d \) is the displacement.
In our given problem, we know:
  • The final velocity \( v = 20 \, \text{m/s} \)
  • The initial velocity \( u = 0 \, \text{m/s} \) because the car starts from rest
  • The displacement \( d = 80 \, \text{m} \)
Using these values in the kinematic equation allows us to calculate the acceleration needed to achieve this movement over the specified distance.
Acceleration Calculation
Acceleration measures how quickly the velocity of an object changes. It is a key piece in understanding how forces cause changes in the motion of objects. The unit of acceleration is meters per second squared (\(\text{m/s}^2\)). To find the acceleration, we use the kinematic equation:
  • \( v^2 = u^2 + 2ad \)
Given the final velocity \( v = 20 \, \text{m/s} \), initial velocity \( u = 0 \, \text{m/s} \), and displacement \( d = 80 \, \text{m} \), we plugged these values into the equation:\[(20)^2 = 0^2 + 2a \times 80\]This simplifies to:\[ 400 = 160a \]Solving for \( a \), we find:\[ a = \frac{400}{160} = 2.5 \, \text{m/s}^2 \]Thus, the car requires an acceleration of \( 2.5 \, \text{m/s}^2 \) to reach the desired velocity of \( 20 \, \text{m/s} \) over the distance of \( 80 \, \text{m} \).
Force Calculation
Once we know the acceleration, we can determine the required force using Newton's Second Law of Motion, which connects force, mass, and acceleration. It is expressed as:
  • \( F = ma \), where \( F \) is the force in newtons, \( m \) is the mass in kilograms, and \( a \) is the acceleration in meters per second squared.
For our car, we have:
  • Mass \( m = 1300 \, \text{kg} \)
  • Acceleration \( a = 2.5 \, \text{m/s}^2 \)
Using these values, we substitute into the formula:\[ F = 1300 \times 2.5 \]This calculation gives us:\[ F = 3250 \, \text{N} \]Hence, a force of \( 3250 \, \text{N} \) is necessary to accelerate the 1300-kg car from rest to a speed of \( 20 \, \text{m/s} \) over a distance of \( 80 \, \text{m} \). This highlights how forces interact with mass and motion, crucial aspects of Newtonian physics.

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Most popular questions from this chapter

A \(10.0\) -kg block is launched up a \(30.0^{\circ}\) inclined plane at a speed of \(20.0 \mathrm{~m} / \mathrm{s}\). As it slides it loses \(200 \mathrm{~J}\) to friction. How far along the incline will it travel before coming to rest?

A block moves up a \(30^{\circ}\) incline under the action of applied forces, three of which are shown in Fig. \(6-2 . \overrightarrow{\mathbf{F}}_{1}\) is horizontal and of magnitude \(40 \mathrm{~N} \cdot \overrightarrow{\mathbf{F}}_{2}\) is normal to the plane and of magnitude \(20 \mathrm{~N}\). \(\overrightarrow{\mathbf{F}}_{3}\) is parallel to the plane and of magnitude \(30 \mathrm{~N}\). Determine the work done by each force as the block (and point of application of each force) moves \(80 \mathrm{~cm}\) up the incline. The component of \(\overrightarrow{\mathbf{F}}_{1}\) along the direction of the displacement is $$ F_{1} \cos 30^{\circ}=(40 \mathrm{~N})(0.866)=34.6 \mathrm{~N} $$ Hence, the work done by \(\overrightarrow{\mathbf{F}}\), is \((34.6 \mathrm{~N})(0.80 \mathrm{~m})=28 \mathrm{~J}\). (Notice that the distance must be expressed in meters.) Because it has no component in the direction of the displacement, \(\overrightarrow{\mathbf{F}}_{2}\) does no work. The component of \(\overrightarrow{\mathbf{F}}_{3}\) in the direction of the displacement is \(30 \mathrm{~N}\). Hence, the work done by \(\overrightarrow{\mathbf{F}}_{3}\) is \((30 \mathrm{~N})\) \((0.80 \mathrm{~m})=24 \mathrm{~J} .\)

A \(0.25\) -hp motor is used to lift a load at the rate of \(5.0 \mathrm{~cm} / \mathrm{s}\). How great a load can it raise at this constant speed? Assume the power output of the motor to be \(0.25 \mathrm{hp}=186.5 \mathrm{~W} .\) In \(1.0 \mathrm{~s}\), the load \(m g\) is lifted a distance of \(0.050 \mathrm{~m}\). Therefore, Work done in \(1.0 \mathrm{~s}=\) (weight) (height change in \(1.0 \mathrm{~s})=(m g)(0.050 \mathrm{~m})\) By definition, Power = Work /Time, and so $$ 186.5 \mathrm{~W}=\frac{(m g)(0.050 \mathrm{~m})}{1.0 \mathrm{~s}} $$ Using \(g=9.81 \mathrm{~m} / \mathrm{s}^{2}\), we find that \(m=381 \mathrm{~kg}\). The motor can lift a load of about \(0.38 \times 10^{3} \mathrm{~kg}\) at this speed.

The driver of a \(1200-\mathrm{kg}\) car notices that the car slows from \(20 \mathrm{~m} / \mathrm{s}\) to \(15 \mathrm{~m} / \mathrm{s}\) as it coasts a distance of \(130 \mathrm{~m}\) along level ground. How large a force opposes the motion?

A \(0.50-\mathrm{kg}\) block slides across a tabletop with an initial velocity of \(20 \mathrm{~cm} / \mathrm{s}\) and comes to rest in a distance of \(70 \mathrm{~cm}\). Find the average friction force that retarded its motion. The \(\mathrm{KE}\) of the block is decreased because of the slowing action of the friction force. That is, Change in \(\mathrm{KE}\) of block \(=\) Work done on block by friction force $$ \frac{1}{2} m v_{f}^{2}-\frac{1}{2} m v_{i}^{2}=F_{\mathrm{f}} s \cos \theta $$ Because the friction force on the block is opposite in direction to the displacement, \(\cos \theta=-1\). Using \(v_{f}=0\), \(v_{i}=0.20 \mathrm{~m} / \mathrm{s}\), and \(s=0.70 \mathrm{~m}\), the above equation becomes $$ 0-\frac{1}{2}(0.50 \mathrm{~kg})(0.20 \mathrm{~m} / \mathrm{s})^{2}=\left(F_{\mathrm{f}}\right)(0.70 \mathrm{~m})(-1) $$ from which \(F_{t}=0.014 \mathrm{~N}\).

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