/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 55 A hypodermic syringe is attached... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A hypodermic syringe is attached to a needle that has an internal radius of \(0.300 \mathrm{mm}\) and a length of \(3.00 \mathrm{cm} .\) The needle is filled with a solution of viscosity $2.00 \times 10^{-3} \mathrm{Pa} \cdot \mathrm{s} ;\( it is injected into a vein at a gauge pressure of \)16.0 \mathrm{mm}$ Hg. Ignore the extra pressure required to accelerate the fluid from the syringe into the entrance of the needle. (a) What must the pressure of the fluid in the syringe be in order to inject the solution at a rate of $0.250 \mathrm{mL} / \mathrm{s} ?$ (b) What force must be applied to the plunger, which has an area of \(1.00 \mathrm{cm}^{2} ?\)

Short Answer

Expert verified
Answer: To find the force applied to the plunger, follow these steps: 1. Convert the flow rate to m^3/s: 0.250 mL/s * 10^(-6) m^3/mL = 0.250 * 10^(-6) m^3/s. 2. Convert the gauge pressure to Pascals: (16.0 mm Hg / 760 mm Hg) * 101325 Pa. 3. Use Poiseuille's law to find the pressure difference: ΔP = (8 * η * L * Q) / (π * r^4). 4. Calculate the pressure in the syringe: P_syringe = P_gauge + ΔP. 5. Calculate the force on the plunger: F = P_syringe * A.

Step by step solution

01

(Step 1: Find the flow rate)

We are given the flow rate is \(0.250 \mathrm{mL} / \mathrm{s}\), which we need to convert to \(\mathrm{m}^3 / \mathrm{s}\) by using the relationship \(\mathrm{mL} = 10^{-6}\mathrm{m}^3\): $$Q=0.250 \times 10^{-6} \,\mathrm{m}^{3}/\mathrm{s}$$
02

(Step 2: Convert pressure to SI units)

The gauge pressure is given as \(16.0 \mathrm{mm}\) Hg. We need to convert it to Pascals (Pa) using the standard atmospheric pressure (\(101325 \mathrm{Pa}\)) and the relationship between mm Hg and atmospheric pressure, which is \(1 \,\mathrm{atm} = 760 \,\mathrm{mm} \, \mathrm{Hg}\): $$P_{gauge} = \frac{16.0}{760}\times 101325 \,\mathrm{Pa}$$
03

(Step 3: Apply Poiseuille's law to find pressure difference)

Recall that the Poiseuille's law states, $$Q = \frac{\Delta P \pi r^4}{8\eta L}$$ Given the flow rate \(Q\), viscosity \(\eta\), internal radius \(r\) and length \(L\) of the needle, we can solve for the pressure difference \(\Delta P\): $$\Delta P = \frac{8\eta LQ}{\pi r^4}$$
04

(Step 4: Calculate pressure in the syringe)

Since the pressure difference \(\Delta P\) is equal to the pressure in the syringe minus the gauge pressure \(P_{gauge}\), we can find the pressure in the syringe: $$P_{syringe} = P_{gauge} + \Delta P$$
05

(Step 5: Calculate the force on the plunger)

We know that the pressure \(P_{syringe}\) is equal to the force on the plunger divided by the area of the plunger \(A\). Hence, we can derive the force on the plunger by multiplying the pressure in the syringe with the area of the plunger: $$F = P_{syringe} \times A$$

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A bug from South America known as Rhodnius prolixus extracts the blood of animals. Suppose Rhodnius prolixus extracts \(0.30 \mathrm{cm}^{3}\) of blood in 25 min from a human arm through its feeding tube of length \(0.20 \mathrm{mm}\) and radius \(5.0 \mu \mathrm{m} .\) What is the absolute pressure at the bug's end of the feeding tube if the absolute pressure at the other end (in the human arm) is 105 kPa? Assume the viscosity of blood is 0.0013 Pa-s. [Note: Negative absolute pressures are possible in liquids in very slender tubes.]
Assume a water strider has a roughly circular foot of radius $0.02 \mathrm{mm} .$ (a) What is the maximum possible upward force on the foot due to surface tension of the water? (b) What is the maximum mass of this water strider so that it can keep from breaking through the water surface? The strider has six legs.
A lid is put on a box that is \(15 \mathrm{cm}\) long, \(13 \mathrm{cm}\) wide, and \(8.0 \mathrm{cm}\) tall and the box is then evacuated until its inner pressure is \(0.80 \times 10^{5} \mathrm{Pa} .\) How much force is required to lift the lid (a) at sea level; (b) in Denver, on a day when the atmospheric pressure is \(67.5 \mathrm{kPa}\) ( \(\frac{2}{3}\) the value at sea level)?
Near sea level, how high a hill must you ascend for the reading of a barometer you are carrying to drop by 1.0 cm Hg? Assume the temperature remains at \(20^{\circ} \mathrm{C}\) as you climb. The reading of a barometer on an average day at sea level is $76.0 \mathrm{cm}$ Hg. (W) tutorial: gauge)
The deepest place in the ocean is the Marianas Trench in the western Pacific Ocean, which is over \(11.0 \mathrm{km}\) deep. On January \(23,1960,\) the research sub Trieste went to a depth of \(10.915 \mathrm{km},\) nearly to the bottom of the trench. This still is the deepest dive on record. The density of seawater is \(1025 \mathrm{kg} / \mathrm{m}^{3} .\) (a) What is the water pressure at that depth? (b) What was the force due to water pressure on a flat section of area \(1.0 \mathrm{m}^{2}\) on the top of the sub's hull?
See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.