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A Charged Battery A typical 12-V car battery can deliver \(7.5 \times 10^{5} \mathrm{C}\) of charge. If the energy supplied by the battery could be converted entirely to kinetic energy, what speed would it give to a \(1400-\mathrm{kg}\) car that is initially at rest?

Short Answer

Expert verified
The speed of the car would be approximately 113.4 m/s.

Step by step solution

01

Identify the Known Values

We are given that the voltage of the car battery is 12 V and it can deliver a charge of \(7.5 \times 10^{5} \mathrm{C}\). The mass of the car is \(1400 \mathrm{kg}\). We need to find the speed of the car once the battery's energy is converted to kinetic energy.
02

Calculate the Energy Supplied by the Battery

The energy \(E\) supplied by the battery can be calculated using the formula \(E = V \times Q\), where \(V\) is the voltage and \(Q\) is the charge. Here, \(E = 12 \text{ V} \times 7.5 \times 10^{5} \text{ C} = 9 \times 10^{6} \text{ J}\).
03

Relate Energy to Kinetic Energy

The energy converted to kinetic energy is given by \( KE = \frac{1}{2} m v^2 \), where \(m\) is the mass of the car and \(v\) is the velocity we want to find. We have \(KE = 9 \times 10^{6} \text{ J}\).
04

Solve for Speed (\(v\))

Set \(KE\) equal to \(9 \times 10^6 = \frac{1}{2} \times 1400 \times v^2\). Simplifying, \(v^2 = \frac{9 \times 10^6 \times 2}{1400}\). Solve for \(v\) to get \(v = \sqrt{\frac{18 \times 10^6}{1400}}\).
05

Compute the Numerical Solution

Calculate \(v = \sqrt{\frac{18 \times 10^6}{1400}}\). This simplifies to \(v = \sqrt{12,857} \approx 113.4 \text{ m/s}\).

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Key Concepts

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

Charge
Charge is essentially a property of matter. It causes it to experience a force when placed in an electromagnetic field. In simpler terms, charge is one of the core elements that define how particles interact with each other.
In the context of our problem, the car battery delivers a large amount of charge, specifically \(7.5 \times 10^{5} \mathrm{C}\). This charge represents the total electric quantity available from the battery to perform work.
Electrons act as carriers that move charge through circuits, and this flow is what we measure as current. Understanding this electric charge and its role in circuits is crucial for grasping how devices like car batteries function and how they are able to provide energy for different operations.
Voltage
Voltage, also known as electric potential difference, is the force that pushes electric charge through a circuit. It is often referred to as electrical pressure.
This is what makes charges flow and do useful work. The voltage of a car battery reflects how much potential energy it can impart to the charge flowing through it. A typical car battery in our example has a voltage of 12 V.
  • Voltage is akin to water pressure in a pipe; higher voltage means greater force to push current.
  • This 12 V tells us the energy each coulomb of charge can transform or transfer.
Understanding voltage is key when evaluating the efficiency and capability of electrical devices and systems.
Energy Conversion
Energy conversion is the process of changing one form of energy into another. In our scenario, the energy stored in the car battery is initially in the form of chemical energy.
When the battery is used, this energy is converted into electrical energy as charge moves through the circuit. Finally, this electrical energy is transformed into kinetic energy, which moves the car.
The formula to calculate this conversion:
\[ E = V \times Q \]
Helps us determine the amount of electrical energy available from a battery.
  • In this problem, the electrical energy was calculated as \(9 \times 10^{6} \text{ J}\).
  • This serves as the kinetic energy that contributes to moving the 1400 kg car.
Grasping how energy can transform from one form to another is vital in physics, especially when dealing with energy efficiencies.
Velocity Calculation
Velocity calculation is crucial to understand how fast an object moves when energy converts into kinetic energy.
Kinetic energy is expressed as \( KE = \frac{1}{2} m v^2 \), where \(m\) is mass and \(v\) is velocity.
To find the car's velocity when the battery's energy is wholly converted into kinetic energy, we rearrange the kinetic energy formula to solve for velocity.
  • We equate the supplied energy to the kinetic energy: \(9 \times 10^6 = \frac{1}{2} \times 1400 \times v^2 \).
  • By solving \(v = \sqrt{\frac{18 \times 10^6}{1400}}\), we get \(v \approx 113.4 \text{ m/s}\).
This tells us how energy translates to motion in real scenarios and the speed at which the energy can move an object of given mass.

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Most popular questions from this chapter

A parallel-plate capacitor is connected to a battery that maintains a constant potential difference \(V\) between the plates. If the plates of the capacitor are pulled farther apart, do the following quantities increase, decrease, or remain the same? (a) The electric field between the plates; (b) the charge on the plates; (c) the capacitance; (d) the energy stored in the capacitor.

Rutherford's Planetary Model of the Atom In 1911 , Ernest Rutherford developed a planetary model of the atom, in which a small positively charged nucleus is orbited by electrons. The model was motivated by an experiment carried out by Rutherford and his graduate students, Geiger and Marsden. In this experiment, they fired alpha particles with an initial speed of \(1.75 \times 10^{7} \mathrm{m} / \mathrm{s}\) at a thin sheet of gold. (Alpha particles are obtained from certain radioactive decays. They have a charge of \(+2 e\) and a mass of \(6.64 \times 10^{-27} \mathrm{kg}\).) How close can the alpha particles get to a gold nucleus (charge \(=+79 e\) ), assuming the nucleus remains stationary? (This calculation sets an upper limit on the size of the gold nucleus. See Chapter 31 for further details.)

Two point charges are placed on the \(x\) axis. The charge \(+2 q\) is at \(x=1.5 \mathrm{m},\) and the charge \(-q\) is at \(x=-1.5 \mathrm{m}\). (a) There is a point on the \(x\) axis between the two charges where the electric potential is zero. Where is this point? (b) The electric potential also vanishes at a point in one of the following regions: region \(1, x\) between \(1.5 \mathrm{m}\) and \(5.0 \mathrm{m} ;\) region \(2, x\) between \(-1.5 \mathrm{m}\) and \(-3.0 \mathrm{m} ;\) region \(3, x\) between \(-3.5 \mathrm{m}\) and \(-5.0 \mathrm{m} .\) Identify the appropriate region. (c) Find the value of \(x\) referred to in part (b).

A spark plug in a car has electrodes separated by a gap of 0.025 in. To create a spark and ignite the air-fuel mixture in the engine, an electric field of \(3.0 \times 10^{6} \mathrm{V} / \mathrm{m}\) is required in the gap. (a) What potential difference must be applied to the spark plug to initiate a spark? (b) If the separation between electrodes is increased, does the required potential difference increase, decrease, or stay the same? Explain. (c) Find the potential difference for a separation of 0.050 in.

To operate a given flash lamp requires a charge of \(32 \mu C .\) What capacitance is needed to store this much charge in a capacitor with a potential difference between its plates of \(9.0 \mathrm{V} ?\)

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