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Variations in the resistivity of blood can give valuable clues about changes in various properties of the blood. Suppose a medical device attaches two electrodes into a 1.5mmdiameter vein at positions role="math" localid="1649141775053" 5.0cmapart. What is the blood resistivity if a 9.0Vpotential difference causes a230μA current through the blood in the vein?

Short Answer

Expert verified

The blood resistivity if a 9.0Vpotential difference causes a localid="1649141831118" 230μAcurrent through the blood in the vein is1.4Ωm.

Step by step solution

01

Given Information

Two electrodes diameterd=1.5mm

Distance=5.0cm

Potential differencelocalid="1649142178730" =9.0V

Current I=230μA

02

Explanation

We can use following equation to find the length:

I=ΔVR

Where Ris resistance. This yields,

R=ΔVI

Here ΔVis potential difference and Iis the current

Calculate the resistivity,

R=ÒÏLA

A, is the area of the cross section of the vein,

Lis the length of vein and ÒÏis resistivity of vein.

The expression for the resistivity is,

ΔVI=ÒÏLA

ÒÏ=ΔVAIL

The diameter of blood vein is 1.5mm.

Convert units of diameter from mmto m

d=(1.5mm)1m1000mm

=1.5×10-3m

Radius of the vein is

r=d2

=1.5×10-3m2

=0.00075m

03

Explanation

Area of blood vein is

A=Ï€r2

=Ï€(0.00075m)2

=1.767×10-6m2

The two electrodes are a length, L, of 5.0cm

Convert units of length from cmto m

L=(5.0cm)1m100cm

=5.0×10-2m

ÒÏ=(9.0V)1.767×10-6m2230×10-6A5.0×10-2m

ÒÏ=1.4Ωm

04

Final Answer 

Therefore, the blood resistivity if a 9.0Vpotential difference causes a 230mAcurrent through the blood in the vein is 1.4Ωm.

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Most popular questions from this chapter

Which, if any, of these statements are true? (More than one may be true.) Explain. Assume the batteries are ideal.

a. A battery supplies the energy to a circuit.

b. A battery is a source of potential difference; the potential difference between the terminals of the battery is always the same.

c. A battery is a source of current; the current leaving the battery is always the same.

The resistivity of a metal increases slightly with increased temperature. This can be expressed as ÒÏ=ÒÏ01+αT-T0, where T0 is a reference temperature, usually 20°C, and a is the temperature coefficient of resistivity.

a. First find an expression for the current I through a wire of length L, cross-section area A, and temperature T when connected across the terminals of an ideal battery with terminal voltage ∆V. Then, because the change in resistance is small, use the binomial approximation to simplify your expression. Your final expression should have the temperature coefficient a in the numerator.

b. For copper, a = 3.9 * 10-3 °C-1 . Suppose a 2.5-m-long, 0.40-mm-diameter copper wire is connected across the terminals of a 1.5 V ideal battery. What is the current in the wire at 20°C?

c. What is the rate, in A/°C, at which the current changes with temperature as the wire heats up?

The two wires in FIGURE P27.62 are made of the same material. What are the current and the electron drift speed in the 2.0-mm-diameter segment of the wire?

Is FIGURE Q27.4 a possible surface charge distribution for a current-carrying wire? If so, in which direction is the current? If not, why not?

The total amount of charge that has entered a wire at time tis given by the expressionQ=(20C)1-e-4(20s), where tis in seconds andt≥0.
a. Find an expression for the current in the wire at timet.
b. What is the maximum value of the current?
c. Graph Iversus tfor the interval 0≤t≤10s.

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