- #1
gelfand
- 40
- 3
Member advised to use the homework template for posts in the homework sections of PF.
Problem :
A car of mass ##m## is parked on a slope.
What does static friction ##\mu_s## have to be for the car not to slide down if
the incline of the hill is ##30## degrees?
*******
For this problem I have the following forces, where the hill is inclined upwards
to the right:
Upwards : normal force of ##mg \cos(\theta)##
Downwards : Force due to gravity of ##mg \cos(\theta)##
Right (so up hill): Resistive Force due to friction ##\mu_s mg \cos(\theta)##
Left (down hill): Force due to gravity : ##mg \sin(\theta)##.
For the car to remain in place I need to have the frictional force to be greater
than the gravitational, if I set these up as
$$
\mu_s mg \cos(\theta) = mg \sin(\theta)
$$
Then reduce to
$$
\mu_s = \tan(\theta)
$$
Where ##\theta = 30## (degrees) , so ##\mu_s = \frac{\sqrt{3}}{3}##, which is around
##0.58##. I *think* that this is a reasonable coefficient for friction? It's less
than 1, though I've not really got anything to go on there.
I'm not sure what else I could do / say about this problem either. I think that
I've considered all the forces, noted that the maximum that friction could be is
that of the equality ##\mu_2 \cos(\theta) = \sin(\theta)## (I've dropped ##mg##
there...)
Static frictional force can change - whereas the kinetic friction is constant.
However - both coefficients ##\mu_s## and ##\mu_k## are themselves constants, so my
equation to find the coefficient ##\mu_s## is valid.
I've attached sketches of this problem as they were requested in the equation.
One other thing that I'm slightly unsure of is the expression for the force of
friction here.
I know that the force of friction is the normal multiplied by the frictional
coefficient. So in this case I have the normal as ##mg \cos(\theta)##, giving
##\mu_s mg \cos(\theta)## as the force of friction. I was slightly unsure because
it's actually ##\sin(\theta)## which is in the direction of the hill here.
Thanks.
A car of mass ##m## is parked on a slope.
What does static friction ##\mu_s## have to be for the car not to slide down if
the incline of the hill is ##30## degrees?
*******
For this problem I have the following forces, where the hill is inclined upwards
to the right:
Upwards : normal force of ##mg \cos(\theta)##
Downwards : Force due to gravity of ##mg \cos(\theta)##
Right (so up hill): Resistive Force due to friction ##\mu_s mg \cos(\theta)##
Left (down hill): Force due to gravity : ##mg \sin(\theta)##.
For the car to remain in place I need to have the frictional force to be greater
than the gravitational, if I set these up as
$$
\mu_s mg \cos(\theta) = mg \sin(\theta)
$$
Then reduce to
$$
\mu_s = \tan(\theta)
$$
Where ##\theta = 30## (degrees) , so ##\mu_s = \frac{\sqrt{3}}{3}##, which is around
##0.58##. I *think* that this is a reasonable coefficient for friction? It's less
than 1, though I've not really got anything to go on there.
I'm not sure what else I could do / say about this problem either. I think that
I've considered all the forces, noted that the maximum that friction could be is
that of the equality ##\mu_2 \cos(\theta) = \sin(\theta)## (I've dropped ##mg##
there...)
Static frictional force can change - whereas the kinetic friction is constant.
However - both coefficients ##\mu_s## and ##\mu_k## are themselves constants, so my
equation to find the coefficient ##\mu_s## is valid.
I've attached sketches of this problem as they were requested in the equation.
One other thing that I'm slightly unsure of is the expression for the force of
friction here.
I know that the force of friction is the normal multiplied by the frictional
coefficient. So in this case I have the normal as ##mg \cos(\theta)##, giving
##\mu_s mg \cos(\theta)## as the force of friction. I was slightly unsure because
it's actually ##\sin(\theta)## which is in the direction of the hill here.
Thanks.