How Does Adding Weight to a Forklift's Forks Affect the Load on the Rear Axle?

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SUMMARY

The discussion focuses on the impact of adding weight to a forklift's forks on the load distribution between the front and rear axles. Participants emphasize the importance of using the moment equation, M = F.d, to analyze the forces acting on the forklift. It is established that the center of gravity (G) remains unchanged, and the load on the rear axle increases as weight (w) is added to the front forks. The correct approach involves taking moments about the front axle to derive the relationship between the weights and normal forces at each axle.

PREREQUISITES
  • Understanding of static equilibrium and moments in physics
  • Familiarity with the concepts of center of gravity and torque
  • Knowledge of normal forces acting on a system
  • Ability to apply the equation M = F.d in practical scenarios
NEXT STEPS
  • Study the principles of static equilibrium in mechanical systems
  • Learn about the calculation of moments and torques in various contexts
  • Explore the effects of load distribution on vehicle dynamics
  • Investigate the role of center of gravity in stability analysis
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Mechanical engineers, forklift operators, and students studying physics or engineering mechanics will benefit from this discussion, particularly those interested in load management and stability in material handling equipment.

longnh
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Homework Statement



A forklift truck of weight W has dimensions shown in the figure below. Its centre of gravity G is mid-way between the front and the rear axles.

9uzmtQB.jpg


When a uniform block of
weight w (w < W) is placed on the front forks as shown, how the load on the rear axle will change?

Homework Equations



Will the truck's center of gravity G change?

The Attempt at a Solution


I tried to use M = F.d, but I don't know which items are constant, and which ones change.

Please help. Thanks in advance.
 
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When taking moments, it helps to choose the axis you take moments about carefully. Where would you think is the best place here?
 
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M = F d is the relevant equation indeed. Do pay attention to the signs !

General remark: before doing 'real work', you can skip answers (c) (because that's not a load but a number) and (d) (it certainly won't increase).

In fact, you can also distinguish between (a) and (b) in a lazy way: what happens with the load if w comes close to W ?

To help you with your 'relevant equation' : G stays in the same place for the truck itself. So there are two torques to consider: from the truck and from the load.
 
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Thank you guys for tipping.

In a lazy way, the answer should be (a). w/2 but I cannot find a solution to that result.

Consider G stays unchanged.

At early state: M1=M2
<=> F1.d = F2.d
<=> W1 = W2 = W/2

When that block is loaded, we have M'1=M'2
<=> F1.d + F.2d = F'2.d
<=> (W/2).d + w.2d = (W'/2).d
<=> :nb):L:L:L
 
longnh said:
Thank you guys for tipping.

In a lazy way, the answer should be (a). w/2 but I cannot find a solution to that result.

Consider G stays unchanged.

At early state: M1=M2
<=> F1.d = F2.d
<=> W1 = W2 = W/2

When that block is loaded, we have M'1=M'2
<=> F1.d + F.2d = F'2.d
<=> (W/2).d + w.2d = (W'/2).d
<=> :nb):L:L:L
Please state what point you are taking moments about. If it is the centre of mass of the truck then you have a distance wrong.
As BvU posted, be careful with signs. Best way is to pick a direction (left or right) as positive and measure each distance from the axis to the force using the appropraite sign. Doing things that way you write that the sum of moments is zero.
Another approach is just to stop and think which moments are clockwise and which are anticlockwise and write that the sum of the clockwise equals the sum of the anticlockwise.
 
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Yes, haruspex, because the truck didn't rotate, sum of counterclockwise moments (front wheels) equals to clockwise moment (at rear wheels). So I have M'1 = M'2 written above.

If I choose an axis with positive direction from left to right, then ∑M = 0 ⇔ (W'/2).d - w.2d - (W/2).d, which is the same as my equation above.

The equation ∑M = M1 - M2 and M1 = M2 are alternative.

The thing that matters is if that block is loaded, is the whole weight of the truck changed, too? Or we consider that w doesn't affect W?
haruspex said:
Please state what point you are taking moments about. If it is the centre of mass of the truck then you have a distance wrong.
As BvU posted, be careful with signs. Best way is to pick a direction (left or right) as positive and measure each distance from the axis to the force using the appropraite sign. Doing things that way you write that the sum of moments is zero.
Another approach is just to stop and think which moments are clockwise and which are anticlockwise and write that the sum of the clockwise equals the sum of the anticlockwise.
 
longnh said:
The thing that matters is if that block is loaded, is the whole weight of the truck changed, too? Or we consider that w doesn't affect W?

Weight means mass times g here, the force of gravity. The weight of the truck itself does not change if load is added.

Consider the moments (torques) of all forces acting on the truck+load system. They are the forces of gravity W and w acting at the centres of mass, and the upward normal forces acting between the ground and the wheels. Load on the rear axle is equal in magnitude with the normal force acting on the real wheel. Choose the front axle and write the moments of all forces with respect to it.
 
longnh said:
Yes, haruspex, because the truck didn't rotate, sum of counterclockwise moments (front wheels) equals to clockwise moment (at rear wheels). So I have M'1 = M'2 written above.

If I choose an axis with positive direction from left to right, then ∑M = 0 ⇔ (W'/2).d - w.2d - (W/2).d, which is the same as my equation above.

The equation ∑M = M1 - M2 and M1 = M2 are alternative.

The thing that matters is if that block is loaded, is the whole weight of the truck changed, too? Or we consider that w doesn't affect W?
You're still not saying what point you are taking moments about. Is it the mass centre of the (unloaded) truck? The front wheels?
 
longnh said:
Yes, haruspex, because the truck didn't rotate, sum of counterclockwise moments (front wheels) equals to clockwise moment (at rear wheels). So I have M'1 = M'2 written above.

If I choose an axis with positive direction from left to right, then ∑M = 0 ⇔ (W'/2).d - w.2d - (W/2).d, which is the same as my equation above.

The equation ∑M = M1 - M2 and M1 = M2 are alternative.

The thing that matters is if that block is loaded, is the whole weight of the truck changed, too? Or we consider that w doesn't affect W?
You're still not saying what point you are taking moments about. Is it the mass centre of the (unloaded) truck? The front wheels?
 
  • #10
I'm talking about the mass center of the unloaded truck.

haruspex said:
You're still not saying what point you are taking moments about. Is it the mass centre of the (unloaded) truck? The front wheels?
 
  • #11
longnh said:
I'm talking about the mass center of the unloaded truck.
Thankyou.
There are a couple of problems with the equation you get in post #4.
First, there are four forces acting on the truck: gravity of the truck, the weight of the load w, and the normal force at each wheel.
Gravity on the truck has no momentabout the truck's mass centre, so you can ignore that. The load on the rear axle is equal to the normal force from the road there. Therefore your F1, F2 should be the normal forces from the road. In that light, reconsider the signs in the equation.
Next, you must not assume that one of those normal forces is unchanged by the load.
By the way, it might be a little quicker if you take moments about the front axle instead. That will avoid bringing the normal force on the front axle into the equation.
 
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  • #12
I might see it now.

I used to think that the pivot was that G point, but I was wrong. If the truck was rotated, the pivot would be the front axle.

At the front axle point: w.d = F2.2d ⇔ F2 = w/2

Thank you!

haruspex said:
Thankyou.
There are a couple of problems with the equation you get in post #4.
First, there are four forces acting on the truck: gravity of the truck, the weight of the load w, and the normal force at each wheel.
Gravity on the truck has no momentabout the truck's mass centre, so you can ignore that. The load on the rear axle is equal to the normal force from the road there. Therefore your F1, F2 should be the normal forces from the road. In that light, reconsider the signs in the equation.
Next, you must not assume that one of those normal forces is unchanged by the load.
By the way, it might be a little quicker if you take moments about the front axle instead. That will avoid bringing the normal force on the front axle into the equation.
 
  • #13
longnh said:
I might see it now.

I used to think that the pivot was that G point, but I was wrong. If the truck was rotated, the pivot would be the front axle.
You can make the pivot point for the equation wheever you like, but some choices are more convenient than others.
Using the mass centre works, but the equation involves w and the normal force at each axle. You then need to use the statics equation for the sum of vertical forces to get a second equation involving the two normal forces at the axles and manipulate the equations to eliminate the one of no interest (the normal force at front axle).
At the front axle point: w.d = F2.2d ⇔ F2 = w/2
That depends what you mean by F2.
If we write F for the new normal force at the rear axle and take moments about the front axle we get an equation involving w, F and W.
 
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