Question
You press a book against a vertical wall. Express the force required to hold the book in place,
F
applied
, in terms of
W
book
and
μ
s
.(1 point)
Responses
F
applied
=
μ
k
W
book
upper F subscript applied baseline equal mu subscript k baseline upper W subscript book baseline
F
applied
=
μ
s
W
book
upper F subscript applied baseline equal mu subscript s baseline upper W subscript book baseline
F
applied
=
W
book
/
μ
s
upper F subscript applied baseline equals upper W subscript book baseline divided by mu subscript s baseline
F
applied
=
W
book
/
μ
k
upper F subscript applied baseline equals upper W subscript book baseline divided by mu subscript k baseline
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F
applied
, in terms of
W
book
and
μ
s
.(1 point)
Responses
F
applied
=
μ
k
W
book
upper F subscript applied baseline equal mu subscript k baseline upper W subscript book baseline
F
applied
=
μ
s
W
book
upper F subscript applied baseline equal mu subscript s baseline upper W subscript book baseline
F
applied
=
W
book
/
μ
s
upper F subscript applied baseline equals upper W subscript book baseline divided by mu subscript s baseline
F
applied
=
W
book
/
μ
k
upper F subscript applied baseline equals upper W subscript book baseline divided by mu subscript k baseline
Skip to navigation
Answers
GPT-4o mini
To hold a book against a vertical wall, you need to apply a force that offsets the gravitational force acting on the book, which is its weight (\( W_{book} \)). The force of static friction that helps to prevent the book from sliding down is defined by the static friction coefficient (\( \mu_s \)) and the normal force (\( F_{applied} \)) that you apply against the wall.
The static friction force (\( F_{friction} \)) can be expressed as:
\[
F_{friction} = \mu_s \times F_{normal}
\]
Since the applied force is also the normal force when pushing the book against the wall, we can replace \( F_{normal} \) with \( F_{applied} \):
\[
F_{friction} = \mu_s \times F_{applied}
\]
For the book to stay in place, this frictional force must be equal to the weight of the book:
\[
F_{friction} = W_{book}
\]
Combining the two equations, we have:
\[
\mu_s \times F_{applied} = W_{book}
\]
To solve for \( F_{applied} \):
\[
F_{applied} = \frac{W_{book}}{\mu_s}
\]
Therefore, the correct expression for the force required to hold the book in place is:
\[
F_{applied} = \frac{W_{book}}{\mu_s}
\]
This corresponds to the option:
**\( F_{applied} = \frac{W_{book}}{\mu_s} \)**
The static friction force (\( F_{friction} \)) can be expressed as:
\[
F_{friction} = \mu_s \times F_{normal}
\]
Since the applied force is also the normal force when pushing the book against the wall, we can replace \( F_{normal} \) with \( F_{applied} \):
\[
F_{friction} = \mu_s \times F_{applied}
\]
For the book to stay in place, this frictional force must be equal to the weight of the book:
\[
F_{friction} = W_{book}
\]
Combining the two equations, we have:
\[
\mu_s \times F_{applied} = W_{book}
\]
To solve for \( F_{applied} \):
\[
F_{applied} = \frac{W_{book}}{\mu_s}
\]
Therefore, the correct expression for the force required to hold the book in place is:
\[
F_{applied} = \frac{W_{book}}{\mu_s}
\]
This corresponds to the option:
**\( F_{applied} = \frac{W_{book}}{\mu_s} \)**