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Suppose that the electric potential outside a living cell is higher than that inside the cell by \(0.070 \mathrm{~V}\). How much work is done by the electric force when a sodium ion (charge \(=+e\) ) moves from the outside to the inside?

Short Answer

Expert verified
The work done by the electric force is \(1.1214 \times 10^{-20} \mathrm{~J}\).

Step by step solution

01

Understanding the Problem

We need to determine the work done by the electric force when a sodium ion, carrying a charge of \(+e\), moves across a potential difference. The potential difference is given as \(0.070 \mathrm{~V}\).
02

Charge of a Sodium Ion

The charge of a sodium ion is equal to the charge of a proton, which is \(+e\). Numerically, this is \(1.602 \times 10^{-19} \mathrm{~C}\).
03

Formula for Work Done by Electric Force

The work done by the electric force can be calculated using the formula \( W = q \Delta V \), where \( W \) is the work done, \( q \) is the charge of the ion, and \( \Delta V \) is the potential difference.
04

Substitute the Values

Substitute the values into the formula: Charge \( q = 1.602 \times 10^{-19} \mathrm{~C} \) and \( \Delta V = 0.070 \mathrm{~V} \). Thus, \( W = (1.602 \times 10^{-19} \mathrm{~C})(0.070 \mathrm{~V}) \).
05

Calculate the Work Done

Calculating the above expression, we get \( W = 1.1214 \times 10^{-20} \mathrm{~J} \). This is the amount of work done by the electric force as the sodium ion moves from outside to inside the cell.

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Key Concepts

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

Sodium Ion
Sodium ions are positively charged particles found in various settings, including within and around living cells. These ions are critical for many biological processes, especially in the transmission of signals in nerve cells. A sodium ion carries a charge equivalent to that of a proton, which is why its charge is denoted as "+e." This means its value is approximately \(1.602 \times 10^{-19} \text{ C}\).

In biological contexts, sodium ions move in and out of cells through specialized pathways created by proteins known as ion channels. The movement of sodium ions is crucial for maintaining cellular functions like nerve impulses, muscle contractions, and even the regulation of water in the body.

Understanding the role of sodium ions in living organisms helps explain how electrical signals travel across neurons and enable us to think, feel, and move.
Work Done by Electric Force
The concept of work is pivotal when discussing electric forces. In physics, work describes what happens when a force moves an object over a distance. For electric forces, this idea translates to the movement of charged particles, like sodium ions, across a potential difference.

When an electric force acts upon a charged particle, it does work if the particle moves. The formula used to calculate this work is \( W = q \Delta V \), where \( W \) is the work done, \( q \) is the charge, and \( \Delta V \) is the potential difference experienced by the charge. Plugging in appropriate values helps determine the energy exchange involved, which is crucial in contexts such as cellular activities and energy metabolism.

In our example, we calculated that the work done by an electric force on a sodium ion moving through a potential difference of \(0.070 \text{ V}\) is \(1.1214 \times 10^{-20} \text{ J}\). This small yet significant amount of work is fundamental to sustaining biological processes.
Potential Difference
Potential difference, often referred to as voltage (V), is the measure of electric potential energy per charge unit between two points. In simpler terms, it tells us how much "push" a charge will receive to move from one point to another.

Within biological systems, cells often maintain a potential difference across their membranes, which is essential for many cellular functions such as the transmission of nerve impulses. In the given exercise, the potential difference was \(0.070 \text{ V}\), with the outside of the cell having a higher potential than the inside.

This potential difference functions like a battery, providing the necessary energy for ions like sodium ions to cross cellular membranes, ensuring proper cell function. Understanding potential difference is key to comprehending how cells maintain internal conditions distinct from their external environment.
Charge of a Proton
The charge of a proton is a fundamental constant in physics. It is a positive charge represented as \(+e\), which numerically equals about \(1.602 \times 10^{-19} \text{ C}\). This charge is considered the basic unit of electric charge in the universe.

In scientific calculations and practical scenarios, the charge of the proton is often used as a reference, especially in the study of ions. Since a sodium ion carries the same charge as a proton, understanding this value is critical when determining the behavior and interaction of ions in electric fields.

For example, in problems like the one described, knowing the charge of a proton allows us to calculate the energy transfers as a sodium ion moves across a potential difference. This basic understanding helps students and scientists predict and manipulate how charged particles move in various fields and environments.

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Most popular questions from this chapter

Two capacitors are identical, except that one is empty and the other is filled with a dielectric \((\kappa=4.50) .\) The empty capacitor is connected to a \(12.0-\mathrm{V}\) battery. What must be the potential difference across the plates of the capacitor filled with a dielectric such that it stores the same amount of electrical energy as the empty capacitor?

Refer to Interactive Solution 19.45 at and Multiple-Concept Example 10 for help in solving this problem. An empty capacitor has a capacitance of \(3.2 \mu \mathrm{F}\) and is connected to a 12-V battery. A dielectric material \((\kappa=4.5)\) is inserted between the plates of this capacitor. What is the magnitude of the surface charge on the dielectric that is adjacent to either plate of the capacitor? (Hint: The surface charge is equal to the difference in the charge on the plates with and without the dielectric.)

Identical point charges of \(+1.7 \mu \mathrm{C}\) are fixed to diagonally opposite corners of a square. A third charge is then fixed at the center of the square, such that it causes the potentials at the empty corners to change signs without changing magnitudes. Find the sign and magnitude of the third charge.

During a particular thunderstorm, the electric potential difference between a cloud and the ground is \(V\) cloud \(-V_{\text {ground }}=1.3 \times 10^{8} \mathrm{~V},\) with the cloud being at the higher potential. What is the change in an electron's electric potential energy when the electron moves from the ground to the cloud?

When you walk across a rug on a dry day, your body can become electrified, and its electric potential can change. When the potential becomes large enough, a spark of negative charges can jump between your hand and a metal surface. A spark occurs when the electric field strength created by the charges on your body reaches the dielectric strength of the air. The dielectric strength of the air is \(3.0 \times 10^{6} \mathrm{~N} / \mathrm{C}\) and is the electric field strength at which the air suffers electrical breakdown. Suppose a spark \(3.0 \mathrm{~mm}\) long jumps between your hand and a metal doorknob. Assuming that the electric field is uniform, find the potential difference \(\left(V_{\mathrm{knob}}-V_{\text {hand }}\right)\) between your hand and the doorknob.

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