Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A75kgwindow cleaner uses a10kgladder that is5.0mlong. He places one end on the ground2.5mfrom a wall, rests the upper end against a cracked window, and climbs the ladder. He is3.0mup along the ladder when the window breaks. Neglect friction between the ladder and window and assume that the base of the ladder does not slip. When the window is on the verge of breaking, what are (a) the magnitude of the force on the window from the ladder, (b) the magnitude of the force on the ladder from the ground, and (c) the angle (relative to the horizontal) of that force on the ladder?

Short Answer

Expert verified

a)Themagnitude of the force on the window from the ladderis.2.8×102N

b)The magnitude of the force on the ladder from the groundis.8.8×102N

c)The angle (relative to the horizontal) of that force on the ladderis71°

Step by step solution

01

Listing the given quantities

Mass of thewindow cleanerM=75kg

Mass of the ladderm=10.0kg

Length of the ladderL=5.0m

Distance from the foot of the ladder to theposition of the window cleaner=3.0m

Distance from the wall to the foot of the ladderd=2.5m

02

Understanding the concept of ladder theory

The forces on the ladder are shown in the diagramF1is the force of the window, horizontal because the window is frictionless.F2andF3are the components of the force of the ground on the ladder. MIs the mass of the window cleaner andis the mass of the ladder.

03

Step 3:Explanation

The man is affected by gravity at a point 3.0mup the ladderand the centre of the ladder experiences the effects of gravity.Let θbe the angle between the ladder and the ground.

\begingatheredcosθ=dLθ=cos-12.55=600

04

Calculation of themagnitude of the force on the window from the ladder

(a)

Since the ladder is in equilibrium the sum of the torques about its foot or any other point vanishes.

Let be thedistance from the foot of the ladder to the position of the window cleaner.

Mgcosθ+mgL2cosθ-F1Lsinθ=0F1=(M+mL2)gcosθLsinθ=(75kg)(3.0m)+(10kg)(2.5m)(9.8m/s2)cos60°(5.0m)sin60°=2.8×102N

The magnitude of the force on the window from the ladderis.2.8×102N

05

Calculation of the magnitude of the force on the ladder from the ground

(b)

The sum of the horizontal forces and the sum of the vertical forces also vanish.

F1-F3=0F2-Mg-mg=0F1=F3=2.8×102NF2=(M+m)g=(75kg+10kg)(9.8m/s2)=8.3×102N

The magnitude of the force of the ground on the ladder is given by the square root of the sum of the squares of its components

F=F22+F32=(2.8×102N)2+(8.3×102N)2=8.8×102N

The magnitude of the force on the ladder from the ground is8.8×102N

06

 Calculation of theangle (relative to the horizontal) of that force on the ladder

(c)

The angle ϕbetween the force and the horizontal is given by

tanϕ=F3F2=(830N)(280N)=2.94ϕ=71°

The angle (relative to the horizontal) of that force on the ladder is71°

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 Vaia!

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

If the (square) beam in fig 12-6aassociated sample problem is of Douglasfir, what must be its thickness to keep the compressive stress on it to16 of its ultimate strength?

Question: ForcesF1,F2andF3 act on the structure of Fig. 12-33, shown in an overhead view. We wish to put the structure in equilibrium by applying a fourth force, at a point such as P. The fourth force has vector componentsFhandFv . We are given that a = 2.0 m,b = 3.0m , c = 1 0 m , F1=20N,F2=10NandF3=5.0NFind (a) Fh , (b) Fv, and (c) d.

A crate, in the form of a cube with edge lengths of 1.2m , contains a piece of machinery; the center of mass of the crate and its contents is located 0.30mabove the crate’s geometrical center. The crate rests on a ramp that makes an angle θwith the horizontal. Asθ is increased from zero, an angle will be reached at which the crate will either tip over or start to slide down the ramp. If the coefficient of static frictionμs between ramp and crate is 0.60(a) Does the crate tip or slide? And (b) at what angle θdoes the crate tip or slide occur? (c) Ifμs=0.70,does the crate tip or slide? And (d) Ifμs=0.70,at what angle u does the crate tip or slide occur?

A uniform cube of side length 8.0 cm rests on a horizontal floor.The coefficient of static friction between cube and floor is m. A horizontal pull Pis applied perpendicular to one of the vertical faces of the cube, at a distance 7.0 cmabove the floor on the vertical midline of the cube face. The magnitude of Pis gradually increased. During that increase, for what values ofμ will the cube eventually (a) begin to slide and (b) begin to tip? (Hint:At the onset of tipping, where is the normal force located?)

A uniform beam is 5.0 mlong and has a mass of 53 kg. In Fig. 12-74, the beam is supported in a horizontal position by a hinge and a cable, with angleθ=60°. In unit-vector notation, what is the force on the beam rom the hinge?

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.

Sign-up for free