/*! 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 8 In a hydraulic press such as the... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

In a hydraulic press such as the one shown in Fig. \(13-3\), the large piston has cross-sectional area \(A_{1}=200 \mathrm{~cm}^{2}\) and the small piston has cross-sectional area \(A_{2}=5.0 \mathrm{~cm}^{2} .\) If a force of \(250 \mathrm{~N}\) is applied to the small piston, find the force \(F_{1}\) on the large piston. By Pascal's principle, Pressure under large piston \(=\) Pressure under small piston \(\quad\) or \(\quad \frac{F_{1}}{A_{1}}=\frac{F_{2}}{A_{2}}\) so that $$F_{1}=\frac{A_{1}}{A_{2}} F_{2}=\frac{200}{5.0} 250 \mathrm{~N}=10 \mathrm{kN}$$ Note that atmospheric pressure acting on both pistons cancels out of the calculation.

Short Answer

Expert verified
The force on the large piston is 10 kN.

Step by step solution

01

Identify Known Values

Given: Large piston area, \( A_1 = 200 \text{ cm}^2 \); Small piston area, \( A_2 = 5.0 \text{ cm}^2 \); Force on small piston, \( F_2 = 250 \text{ N} \). We need to find the force, \( F_1 \), on the large piston.
02

Set Up the Problem

According to Pascal's principle, the pressure applied on the small piston must equal the pressure on the large piston. Mathematically, this is expressed as: \( \frac{F_1}{A_1} = \frac{F_2}{A_2} \).
03

Rearrange the Formula to Solve for Force on Large Piston

We know that \( F_1 = \frac{A_1}{A_2} \cdot F_2 \). This relationship is derived from equating the pressures as mentioned in the principle.
04

Substitute the Known Values i

Input the known values into the equation derived: \( F_1 = \frac{200}{5.0} \cdot 250 \text{ N} \).
05

Calculate the Force

Perform the calculation: \( F_1 = 40 \cdot 250 \text{ N} \). This results in \( F_1 = 10,000 \text{ N} \) or \( 10 \text{ kN} \).

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!

Key Concepts

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

Hydraulic Press
A hydraulic press is an interesting machine that uses a simple concept to generate large amounts of force. It operates based on Pascal's Principle, which states that when pressure is applied to a confined fluid, the pressure change is transmitted undiminished throughout the fluid. A hydraulic press usually consists of two pistons of different sizes, connected by a tube filled with hydraulic fluid. When a force is applied to the smaller piston, it creates pressure in the fluid. - **Large Area Impact:** The large piston, having a much larger surface area, responds with an increase in force. This allows the press to lift or compress heavy objects with ease, making it valuable in many industrial applications.
- **Applications:** Hydraulic presses are used in car repairs to bend or straighten metal parts, in the recycling industry to compress waste, and even in making heavy machinery parts.
Pressure Calculation
Pressure calculation in a hydraulic press is a critical step to understand how these devices function. Pressure is defined as the force applied per unit area, and it remains constant throughout the fluid in a closed system as per Pascal's Principle. In our given exercise, we're working with pressures on small and large pistons.- **Equation:** Pressure under each piston can be expressed mathematically as: \[ \text{Pressure} = \frac{\text{Force}}{\text{Area}} \]- **Equal Pressures:** Hence, the pressures on both pistons are equal: \[ \frac{F_1}{A_1} = \frac{F_2}{A_2} \] where: - \( F_1 \) is the force on the large piston - \( A_1 \) is the area of the large piston - \( F_2 \) is the force on the small piston - \( A_2 \) is the area of the small piston.
Understanding these calculations helps in designing systems where force multiplication is needed, leveraging mechanical advantages effectively.
Force Calculation
Calculating the force exerted by the large piston in a hydraulic press setup is straightforward once you understand the principles. Thanks to Pascal's Principle, we know that if we have two different piston sizes, altering the force applied to one will change the force outputted by the other.In the exercise, the following was processed:- **Initial Steps:** Start by applying the equation where pressure under small and large pistons are equal: \[ F_1 = \frac{A_1}{A_2} \times F_2 \]- **Derived Formula:** This formula reflects how force can be increased by using a larger piston surface area. - Given: Small piston force, \( F_2 = 250 \text{ N} \) - Small piston area, \( A_2 = 5.0 \text{ cm}^2 \) - Large piston area, \( A_1 = 200 \text{ cm}^2 \)- **Calculation:** - Substituting these values, we calculate \( F_1 \): \[ F_1 = \frac{200}{5.0} \times 250 = 10,000 \text{ N} \] or \( 10 \text{ kN} \)This calculation shows the dramatic increase in force achieved, highlighting the effectiveness of hydraulic systems in real-world applications.

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

Downward forces of \(45.0 \mathrm{~N}\) and \(15.0 \mathrm{~N}\), respectively, are required to keep a plastic block totally immersed in water and in oil, respectively. If the volume of the block is \(8000 \mathrm{~cm}^{3}\), find the density of the oil.

Find the density \(\rho\) of a fluid at a depth \(h\) in terms of its density \(\rho_{0}\) at the surface. If a mass \(m\) of fluid has volume \(V_{0}\) at the surface, then it will have volume \(V_{0}-\Delta V\) at a depth \(h\). The density at depth \(h\) is then $$ \rho=\frac{m}{V_{0}-\Delta V} \quad \text { while } \quad \rho_{0}=\frac{m}{V_{0}} $$ which gives $$ \frac{\rho}{\rho_{0}}=\frac{V_{0}}{V_{0}-\Delta V}=\frac{1}{1-\left(\Delta V / V_{0}\right)} $$ However, from Chapter 12, the bulk modulus is \(B=P /\left(\Delta V / V_{0}\right)\) and so \(\Delta V / V_{0}=P / B\). Making this substitution, we obtain $$ \frac{\rho}{\rho_{0}}=\frac{1}{1-P / B} $$ If we assume that \(\rho\) is close to \(\rho_{0}\), then the pressure at depth \(h\) is approximately \(\rho_{0} g h\), and so $$ \frac{\rho}{\rho_{0}}=\frac{1}{1-\left(\rho_{0} g h / B\right)} $$

How high would water rise in the essentially open pipes of a building if the water pressure gauge shows the pressure at the ground floor to be \(270 \mathrm{kPa}\) (about \(40 \mathrm{lb} / \mathrm{in.}^{2}\) )? Water pressure gauges read the excess pressure just due to the water, that is, the difference between the absolute pressure in the water and the pressure of the atmosphere. The water pressure at the bottom of the highest column that can be supported is \(270 \mathrm{kPa}\). Therefore, \(P=\rho_{w} g h\) gives $$ h=\frac{P}{\rho_{w} g}=\frac{2.70 \times 10^{5} \mathrm{~N} / \mathrm{m}^{2}}{\left(1000 \mathrm{~kg} / \mathrm{m}^{3}\right)\left(9.81 \mathrm{~m} / \mathrm{s}^{2}\right)}=27.5 \mathrm{~m} $$

Determine the unbalanced force acting on an iron ball \(\left(r=1.5 \mathrm{~cm}, \rho=7.8 \mathrm{~g} / \mathrm{cm}^{3}\right)\) when just released while totally immersed in \((a)\) water and \((b)\) mercury \(\left(\rho=13.6 \mathrm{~g} / \mathrm{cm}^{3}\right) .\) What will be the initial acceleration of the ball in each case?

A glass of water has a \(10-\mathrm{cm}^{3}\) ice cube floating in it. The glass is filled to the brim with cold water. By the time the ice cube has completely melted, how much water will have flowed out of the glass? The sp gr of ice is \(0.92\).

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.