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Zorluk: OrtaLevers and Fulcrums

A maintenance crew uses a horizontal boom mounted on a utility truck to lift a 600 N600 \text{ N} generator. The boom pivots at a hinge on the truck bed. A vertical hydraulic cylinder supports the boom, attaching exactly 1.0 m1.0 \text{ m} from the hinge. The generator hangs from the far end of the boom, 4.0 m4.0 \text{ m} from the hinge. Assuming the weight of the boom itself is negligible, how much upward force must the hydraulic cylinder apply to hold the generator stationary, and what class of lever does this system represent?

  1. 2400 N2400 \text{ N}; third-class leverCevap
  2. B
    150 N150 \text{ N}; second-class lever
  3. C
    1800 N1800 \text{ N}; third-class lever
  4. D
    2400 N2400 \text{ N}; first-class lever

Cevap

2400 N2400 \text{ N}; third-class lever
The system represents a third-class lever because the effort force (the hydraulic cylinder) is applied between the fulcrum (the hinge) and the load (the generator). To maintain static equilibrium, the counterclockwise torque provided by the cylinder must perfectly equal the clockwise torque from the generator. The generator creates a torque of 600 N×4.0 m=2400 N⋅m600 \text{ N} \times 4.0 \text{ m} = 2400 \text{ N}\cdot\text{m}. Therefore, the cylinder must apply 2400 N2400 \text{ N} of force at a distance of 1.0 m1.0 \text{ m} to balance the system (2400 N×1.0 m=2400 N⋅m2400 \text{ N} \times 1.0 \text{ m} = 2400 \text{ N}\cdot\text{m}).

Adım Adım Çözüm

1
Identify the lever class based on the arrangement of the fulcrum, effort, and load.
The effort force (hydraulic cylinder) is located between the fulcrum (hinge) and the load (generator). This arrangement defines a third-class lever.
Determining the lever arrangement is essential to properly visualize the system and answers the classification part of the question.
2
Set up the torque balance equation (principle of moments) around the fulcrum.
To remain stationary, upward torque must equal downward torque: Feffort×deffort=Fload×dloadF_{\text{effort}} \times d_{\text{effort}} = F_{\text{load}} \times d_{\text{load}}
A lever in static equilibrium must have balanced rotational forces acting around its pivot point.
3
Substitute the known distances and forces into the equation to solve for the effort force.
Feffort×1.0 m=600 N×4.0 mF_{\text{effort}} \times 1.0 \text{ m} = 600 \text{ N} \times 4.0 \text{ m}, which simplifies to Feffort=2400 NF_{\text{effort}} = 2400 \text{ N}.
Applying the specific measurements yields the precise upward force required by the cylinder.

Anahtar Kavram

Third-Class Levers and Torque Balance
Tahmini Süre:1m 15s
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