Calculating Torque with Vectors at an Angle

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lukatwo
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Homework Statement


So I was wondering how do we account for vectors that are at a certain angle. The problem that I'm having with the picture is: if I was calculating torque from point B, how would I account for the vector G.
Diagram of a truck parked on an inclined plane at angle α, with center of gravity T, weight vector G acting down from point B, support reactions G1 at wheel A and G2 at wheel B, and distances l1 and l2 marked along the slope.


Homework Equations





The Attempt at a Solution


I've tried taking the component that's vertical to the slope, but in that case what is the lever arm? Is it where the vector G crosses the slope(point D)?
 
lukatwo said:

Homework Statement


So I was wondering how do we account for vectors that are at a certain angle. The problem that I'm having with the picture is: if I was calculating torque from point B, how would I account for the vector G.
Diagram of a truck parked on an inclined plane at angle α, with center of gravity T, weight vector G, support reactions G1 at wheel A and G2 at wheel B, and distances l1 and l2 marked along the slope.


Homework Equations





The Attempt at a Solution


I've tried taking the component that's vertical to the slope, but in that case what is the lever arm? Is it where the vector G crosses the slope(point D)?
Try taking the component that's perpendicular to the ramp (incline).

Do you know about the line of action for a force -- in this case force G ?
 
I've tried taking the perpendicular component, but not sure what the lever arm is. I'm not sure how to determine the line of action.
 
lukatwo said:
I've tried taking the perpendicular component, but not sure what the lever arm is. I'm not sure how to determine the line of action.

By extending the force T, you can see that it will contact point D. So it is like you're applying the force T directly on point D and the lever arm will be BD. Then take the perpendicular component of force T relative to the slope.

You can always check.
If we assume that BT is perpendicular to force T (note: BT is the dist. bet. B and T)
From the figure, the τ = T*(BT) . But, BT = BDsin(90-α). Therefore τ = T*(BDsin(90-α)) [1].
Returning to your problem, τ = Txr where r is the lever arm. The perpendicular component of T is Tsin(90-α). Therefore τ = Tsin(90-α)*r = T*(BDsin(90-α)) from [1]. Therefore r = BD.
 
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