Chapter 2 Problems
1.
Problem Statement 1
Solution:
First, let’s break down the forces into x and y components. If we let positive x be to the right, then we see that “you” are pushing at an angle of 200∘ counter-clockwise from positive x, while “friend” is pusing at an angle of 135∘ counter-clockwise from positive x. Therefore, we have
youxyouyfriendxfriendy=350N(cos200∘)≈−329N,=350N(sin200∘)≈−120N,=450N(cos135∘)≈−318N,=450N(sin135∘)≈318N.
From this, we get the resultant force
FxFy≈−329N−318N=−647N,≈−120N+318N=198N.
Comparing this to the force of friction, we see that a 145 kg mass will produce a weight force of 145 kg(9.8 m/s2)=1421N, so the maximun magnitude of our friction force will be 0.45(1421N)≈639N. Since this is less than our resultant force, yes, it will move.
2.
Problem Statement 2
Solution:
We are given the mass of the skier, the angle of the slope, the magnitude and direction of air resistance, the dynamic friction between skis and snow, and are asked to calculate the resultant force assuming the skier is sliding straight down the slope. Let the
x-axis be parallel to the slope, with the skier traveling in the positive
x direction. Now, since we are told that the skier is traveling straight down the slope, we know that the acceleration (and therefore net force) along the
y-axis must be zero, so we solve for the
x compontents of our three forces: gravity, friction, and air resistance.
The force of gravity on the skier will act 30∘ from the y-axis in the fourth cartesian quadrant, or 300∘ from the x-axis. Therefore, its x component will be
60 kg(9.8 m/s2)(cos300∘)=294N.
and its y component will be
60 kg(9.8 m/s2)(sin300∘)≈−509.2N.
Since the normal force from the ground will be equal in magnitude to this y component, the force of surface friction will be
0.08(−509.2N)≈−40.7.
Combining these with the air friction of 10N gives the resultant force
294N−40.7N−10N=243.3N
in the positive x direction, or 243.3N at 30∘ below horizontal .
3.
Problem Statement 3
Solution:
Let the
y-axis be parallel to the tibia, so that the
x component of our resultant force equals the shear force, and the
y component equals the compressive force. Let the femur be
60∘ counter-clockwise from the positive
x-axis (so that positive
x is posterior and positive
y is superior). Now, in degrees counter-clockwise from positive
x, we have the force of the gastroc at
87∘, force of hamstrings at
60∘, and force of quadriceps at
105∘.
Therefore, the force of the gastroc is
gastrocxgastrocy=780N(cos87∘)≈40.8N,=780N(sin87∘)≈778.9N,
the force of the hamstrings is
hamstringsxhamstringsy=790N(cos60∘)=395N,=790N(sin60∘)≈684.2N,
and the force of the quadriceps is
quadricepsxquadricepsy=1650N(cos105∘)≈−427.1N,=1650N(sin105∘)≈1593.8N.
Summing these up, we have our resultant force as
resultantxresultanty≈40.8N+395N−427N=8.8N,≈778.9N+684.2N+1593.8N=3056.9N.
Therefore, we have
compression=3056.9N and
shear=8.8N .