Figure Before: V 0 = 0° P < 1 of 6 After: ㄧㄢˊˋ F P Course Home - Google Chrome 1m mylabmastering.pearson.com/?courseld=12611274&key=13537117491744514152152024#/ Course Home Review Constants | Periodic Table TACTICS BOX 10.1 Calculating the work done by a constant force Direction of force relative to displacement Angles and work done Sign of W Energy transfer 0 = 0° The force is in the direction of motion. ( Figure 1) COS = 1 + The block has its greatest positive acceleration. Kinetic energy K increases the most: Maximum energy is transferred to the system. W = Fd The component of force parallel to the displacement is less than F. (Figure 2) 0 < 90° + W = Fd cos 0 The block has a smaller positive acceleration. K increases less: Moderate energy is transferred to the system. 0 = 90° There is no component of force in the direction of motion. (Figure 3) COS = 0 0 The block moves at constant speed. There is no change in K: No energy is transferred. W = 0 The component of force parallel to the displacement is opposite to the motion. ( Figure 4) 0 > 90° W = Fd cos 0 0 = 180° The force is directly opposite to the motion. ( Figure 5) cos = 1 The block slows down, and K decreases: Moderate energy is transferred out of the system. The block has its greatest deceleration. K decreases the most Maximum energy is transferred out of the system. W =-Fd A box of weight w = 2.0 N accelerates down a rough plane that is inclined at an angle = 30° above the horizontal, as shown (Figure 6). The normal force 1.7 N, the coefficient of kinetic friction between the box and the plane is = 0.30, and the displacement d of the acting on the box has a magnitude 7 = box is 1.8 m down the inclined plane. Part A What is the work Ww done on the box by the weight of the box? 66°F Sunny л 3:04 PM 3/15/2024 島

College Physics
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ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
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Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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Physics help!

  • what is the work Wn done on the box by the normal force?

so find Wn=____J

 

* hint given background information  "the work Ww done in the box of weight of the box is Ww= 1.8 J"

 

  • next find the work of Wfk done on the box by the force of kinetic friction
    give your answer in:

Wfk=___J

 

 

i have attached supporting details at the bottom.

Figure
Before:
V
0 = 0°
P
<
1 of 6
After:
ㄧㄢˊˋ
F
Transcribed Image Text:Figure Before: V 0 = 0° P < 1 of 6 After: ㄧㄢˊˋ F
P Course Home - Google Chrome
1m
mylabmastering.pearson.com/?courseld=12611274&key=13537117491744514152152024#/
Course Home
<Week 10_2: Energy
Tactics Box 10.1 Calculating the Work Done by a Constant Force
Learning Goal:
To practice Tactics Box 10.1 Calculating the work done by a
constant force.
To find the work done on an object by a force, begin with a visual
overview and follow Tactics Box 10.1.
Recall that the work W done by a constant force F at an angle
to the displacement d is
WFd cos 0.
The vector magnitudes F and d are always positive, so the sign
of W is determined entirely by the angle between the force and
the displacement.
Type here to search
Hi
Help
1 of 6
>
Review Constants | Periodic Table
TACTICS BOX 10.1 Calculating the work done by a constant force
Direction of force relative to displacement
Angles and
work done
Sign of
W
Energy transfer
0
= 0°
The force is in the direction of motion. (
Figure 1)
COS
=
1
+
The block has its greatest positive acceleration. Kinetic energy K
increases the most: Maximum energy is transferred to the system.
W
=
Fd
The component of force parallel to the
displacement is less than F. (Figure 2)
0
<
90°
+
W
=
Fd cos 0
The block has a smaller positive acceleration. K increases less:
Moderate energy is transferred to the system.
0
= 90°
There is no component of force in the direction
of motion. (Figure 3)
COS
=
0
0
The block moves at constant speed. There is no change in K: No
energy is transferred.
W
=
0
The component of force parallel to the
displacement is opposite to the motion. (
Figure 4)
0
>
90°
W
=
Fd cos 0
0
=
180°
The force is directly opposite to the motion. (
Figure 5)
cos
=
1
The block slows down, and K decreases: Moderate energy is
transferred out of the system.
The block has its greatest deceleration. K decreases the most
Maximum energy is transferred out of the system.
W
=-Fd
A box of weight w = 2.0 N accelerates down a rough plane that is inclined at an angle = 30° above the horizontal, as shown (Figure 6). The normal force
1.7 N, the coefficient of kinetic friction between the box and the plane is = 0.30, and the displacement d of the
acting on the box has a magnitude 7 =
box is 1.8 m down the inclined plane.
Part A
What is the work Ww done on the box by the weight of the box?
66°F Sunny
л
3:04 PM
3/15/2024
島
Transcribed Image Text:P Course Home - Google Chrome 1m mylabmastering.pearson.com/?courseld=12611274&key=13537117491744514152152024#/ Course Home <Week 10_2: Energy Tactics Box 10.1 Calculating the Work Done by a Constant Force Learning Goal: To practice Tactics Box 10.1 Calculating the work done by a constant force. To find the work done on an object by a force, begin with a visual overview and follow Tactics Box 10.1. Recall that the work W done by a constant force F at an angle to the displacement d is WFd cos 0. The vector magnitudes F and d are always positive, so the sign of W is determined entirely by the angle between the force and the displacement. Type here to search Hi Help 1 of 6 > Review Constants | Periodic Table TACTICS BOX 10.1 Calculating the work done by a constant force Direction of force relative to displacement Angles and work done Sign of W Energy transfer 0 = 0° The force is in the direction of motion. ( Figure 1) COS = 1 + The block has its greatest positive acceleration. Kinetic energy K increases the most: Maximum energy is transferred to the system. W = Fd The component of force parallel to the displacement is less than F. (Figure 2) 0 < 90° + W = Fd cos 0 The block has a smaller positive acceleration. K increases less: Moderate energy is transferred to the system. 0 = 90° There is no component of force in the direction of motion. (Figure 3) COS = 0 0 The block moves at constant speed. There is no change in K: No energy is transferred. W = 0 The component of force parallel to the displacement is opposite to the motion. ( Figure 4) 0 > 90° W = Fd cos 0 0 = 180° The force is directly opposite to the motion. ( Figure 5) cos = 1 The block slows down, and K decreases: Moderate energy is transferred out of the system. The block has its greatest deceleration. K decreases the most Maximum energy is transferred out of the system. W =-Fd A box of weight w = 2.0 N accelerates down a rough plane that is inclined at an angle = 30° above the horizontal, as shown (Figure 6). The normal force 1.7 N, the coefficient of kinetic friction between the box and the plane is = 0.30, and the displacement d of the acting on the box has a magnitude 7 = box is 1.8 m down the inclined plane. Part A What is the work Ww done on the box by the weight of the box? 66°F Sunny л 3:04 PM 3/15/2024 島
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