Consider a phospholipid vesicle containing \(10 \mathrm{m} M \mathrm{Na}^{+}\) ions. The vesicle is bathed in a solution that contains \(52 \mathrm{mM} \mathrm{Na}^{+}\) ions, and the electrical potential difference across the vesicle membrane \(\Delta \psi=\psi_{\text {outside }}-\psi_{\text {inside }}=-30 \mathrm{mV} .\) What is the electrochemical potential at \(25^{\circ} \mathrm{C}\) for \(\mathrm{Na}^{+}\) ions?

Short Answer

Expert verified
The electrochemical potential for Na+ ions at 25°C is calculated using the Nernst equation. After substituting the given values into the equation, one can solve for the electrochemical potential.

Step by step solution

01

Understanding the problem

We need to calculate the electrochemical potential of sodium ions inside a phospholipid vesicle surrounded by a solution with a different concentration of the same ions. Additionally, an electrical potential difference across the membrane has been provided. Note that the term 'electrochemical potential', used in the context of ions across a membrane, is derived from the Nernst equation.
02

Using Nernst Equation

The Nernst equation gives the electrochemical potential difference (Δμ) between two points in terms of the ion's valence (z), Temperature (T), Faraday's constant (F), universal gas constant (R), charge on an electron (e), concentration on the inside ([Cin]) and the outside ([Cout]) and the electrical potential (Δψ). The Nernst equation can be written in the form: Δμ= RT/zF ln([Cout]/[Cin]) + zFΔψ
03

Calculating quantities

Substitute the values into the equation. T = 298.15 K (temperature in Kelvin), R = 8.314 J mol^-1K^-1 (universal gas constant), F = 96485 C mol^-1 (Faraday's constant), z = +1 (valence of Na+), [Cout] = 52 mM, [Cin] = 10 mM, Δψ = -30 mV = -0.03V (Electrical potential difference converted to volts).
04

Calculating Electrochemical Potential

Putting the values into the Nernst equation to find the electrochemical potential: Δμ= (8.314 x 298.15/96485)ln(52/10) + 96485 x -0.03

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Key Concepts

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

Nernst Equation
The Nernst equation is fundamental to understanding the behavior of ions in different environments, shaping our comprehension of biochemical and physical processes. Simply put, it relates the concentration of an ion on both sides of a membrane to the voltage across the membrane.

At the core, the Nernst equation can be expressed as: \[\Delta\mu = \frac{RT}{zF} \ln\left(\frac{[C_{out}]}{[C_{in}]}\right) + zF\Delta\psi\]One need not be daunted by the scientific symbols within the equation. Here, \(\Delta\mu\) represents the electrochemical potential difference for a specific ion, \(R\) is the universal gas constant, and \(T\) is the temperature in Kelvin. The valence of the ion is denoted by \(z\), and \(F\) stands for Faraday's constant, which represents the charge per mole of electrons. Importantly, \([C_{out}]\) and \([C_{in}]\) are the ion concentrations outside and inside the membrane, while \(\Delta\psi\) is the electrical potential difference across it.

To utilize this equation for problem-solving, remember to convert temperatures to Kelvin and potentials to Volts. With the correct substitution of values, the Nernst equation unveils the electrochemical potential difference effectively.
Phospholipid Vesicle
Phospholipid vesicles are spherical packets composed of lipid molecules, pivotal in studying cellular processes, including how substances move across biological membranes. They are essentially a simplified model of cell membranes, allowing us to explore the movement of ions such as sodium (\(Na^+\)).

Each vesicle has an 'inside' and 'outside', mimicking the interior and exterior of a cell. When we consider ion movement across the vesicle's membrane, we're looking at a scenario analogous to ion transport in living cells. They're not just scientific curiosities but are vital tools in understanding how drugs get into cells or how nerve cells communicate with each other.

When working with vesicles in our calculations, identifying the concentration of ions inside and outside is crucial, as this sets the stage for the creation of an ion concentration gradient, directly influencing the membrane potential and, thus, the transport of ions.
Membrane Potential
Now let's delve into the concept of membrane potential, which is the voltage difference between the interior and the exterior of a phospholipid vesicle or a cell. This electrical potential difference is critical for activities such as nerve transmission and muscle contraction.

Membrane potential arises due to the unequal distribution of ions across the cellular or vesicle membrane. In the exercise provided, a negative membrane potential as indicates that the inside of the vesicle is more negative in relation to the outside.

This difference in voltage is pivotal for biological functions. It's the driving force behind the movement of ions, which, in turn, can generate electrical signals in nerve and muscle cells or facilitate the uptake of nutrients and expulsion of waste in all cell types. Therefore, when we calculate the electrochemical potential, including the membrane potential as part of the equation enriches our comprehension of the scenario at hand.
Ion Concentration Gradient
An ion concentration gradient refers to the variation in the concentration of ions across a membrane. It's a form of potential energy that can be harnessed by cells to do work, such as transmitting signals or moving substances against another gradient.

In the context of our exercise, there's a concentration gradient for \(Na^+\) ions across the membrane of the vesicle, with a higher concentration of ions in the bathing solution compared to inside the vesicle. The existence of this gradient implies that ions will tend to move from an area of higher concentration to one of lower concentration, a process known as diffusion.

This gradient is a driving force that, when combined with membrane potential, influences the direction and magnitude of ion movement across the membrane. In our exercise's solution, the gradient supplies part of the necessary information to utilize the Nernst equation. It becomes evident that understanding how to calculate the ion concentration gradient is not only key to solving this problem but is also crucial for a deeper understanding of various physiological processes.

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Most popular questions from this chapter

In the description of the mechanism of proton transport by bacteriorhodopsin, we find that light-driven conformation changes promote transmembrane proton transport. Suggest at least one reason for this behavior. In molecular terms, how could a conformation change facilitate proton transport?

Proline residues are almost never found in short \(\alpha\) -helices; nearly all transmembrane \(\alpha\) -helices that contain proline are long ones (about \(20 \text { residues }) .\) Suggest a reason for this observation.

Sucrose gradients for separation of membrane proteins must be able to separate proteins and protein-lipid complexes having a wide range of densities, typically 1.00 to \(1.35 \mathrm{g} / \mathrm{mL}\) a. Consult reference books (such as the CRC Handbook of Biochemistry \()\) and plot the density of sucrose solutions versus percent sucrose by weight (g sucrose per 100 g solution), and versus percent by volume (g sucrose per \(100 \mathrm{mL}\) solution). Why is one plot linear and the other plot curved? b. What would be a suitable range of sucrose concentrations for separation of three membrane-derived protein-lipid complexes with densities of \(1.03,1.07,\) and \(1.08 \mathrm{g} / \mathrm{mL} ?\)

As described in this chapter, proline introduces kinks in transmembrane \(\alpha\) -helices. What are the molecular details of the kink, and why does it form? A good reference for this question is von Heijne, G. 1991\. Proline kinks in transmembrane \(\alpha\) -helices. Journal of Molecular Biology \(218: 499-503 .\) Another is Barlow, D. \(\mathrm{J}\)., and Thornton, J. M., \(1988 .\) Helix geometry in proteins. Journal of Molecular Biology \(201: 601-619\)

In this chapter, we have examined coupled transport systems that rely on ATP hydrolysis, on primary gradients of \(\mathrm{Na}^{+}\) or \(\mathrm{H}^{+},\) and on phosphotransferase systems. Suppose you have just discovered an unusual strain of bacteria that transports rhamnose across its plasma membrane. Suggest experiments that would test whether it was linked to any of these other transport systems.

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