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The figure below shows a metal rule L and weight 7N pivoted at the other shown below. Calculate the angle made by the weight Plank.

Physics

ScanSolve AI Answer

Answer

50.15∘50.15^\circ

Step-by-step solution

4 steps

Okay, Ismaella, let's break down this problem step-by-step, imagining we're reading from an "ordinary person's book" on how things balance.

First, let's understand what's happening in the picture. We have a metal rule (think of it like a long, flat plank) that is balanced. It's pivoted at one end, which means it can rotate around that point, like a seesaw on its fulcrum. For it to stay still and not rotate, all the "turning effects" on it must cancel each other out.

The Goal: We need to find the angle (θ\theta) this plank makes with the flat ground (the horizontal) when it's perfectly balanced.

Here's what we know from the picture and text:

  • The Plank: It has a total length, let's call it LL.
  • Pivot Point (O): It's at the left end of the plank.
  • Plank's Own Weight: 7 N7 \text{ N}. For a uniform plank, its weight acts right in the middle, so at a distance of L2\frac{L}{2} from the pivot. This weight always pulls straight down.
  • Force 1: A 4 N4 \text{ N} force is pushing on the plank. It's applied at an angle of 30∘30^\circ below the plank. From the diagram, it looks like this force is applied at the very end of the plank, so its distance from the pivot is LL.
  • Force 2: An 8 N8 \text{ N} force is also pushing on the plank. It's applied at an angle of 45∘45^\circ below the plank. It's applied at a point that is 14L\frac{1}{4}L from the right end, which means it's 34L\frac{3}{4}L from the pivot (since L−14L=34LL - \frac{1}{4}L = \frac{3}{4}L).

The Big Idea: Rotational Balance (Equilibrium)

For the plank to be balanced and not spinning, the "turning effects" (which we call moments or torques) that try to spin it one way must be equal to the "turning effects" that try to spin it the other way.

  • What is a Moment? It's how much a force tries to make something rotate. You calculate it by multiplying the force by the perpendicular distance from the pivot to where the force is pushing. If the force is at an angle, we only use the part of the force that is perpendicular to the plank, or the perpendicular distance to the line where the force is acting.

Let's assume the plank makes an angle θ\theta with the horizontal ground.


  1. Identify Forces and Their "Turning Directions"

    We'll look at each force and decide if it tries to turn the plank clockwise (like a clock hand moving forward) or anti-clockwise (the opposite direction).

    • Plank's Weight (7 N): This force pulls straight down at the middle of the plank. It will try to make the plank rotate clockwise around the pivot O.
    • 4 N Force: This force is pushing downwards and to the left, at 30∘30^\circ to the plank. It will also try to make the plank rotate clockwise around the pivot O.
    • 8 N Force: This force is pushing downwards and to the right, at 45∘45^\circ to the plank. It will try to make the plank rotate anti-clockwise around the pivot O.

  2. Calculate the "Turning Effect" (Moment) for Each Force

    We'll calculate the moment for each force around the pivot O. Remember, Moment = Force ×\times Perpendicular Distance.

    • Moment from the 4 N force (M1M_1):

      • Force: 4 N4 \text{ N}.
      • Distance from pivot: LL (we are assuming the 'l' in the diagram means the full length LL from the pivot, as this is common in such problems and makes it solvable).
      • Angle: The force is 30∘30^\circ to the plank. The part of this force that causes rotation is 4sin⁡(30∘)4 \sin(30^\circ).
      • Calculation: M1=4 N×L×sin⁡(30∘)M_1 = 4 \text{ N} \times L \times \sin(30^\circ) M1=4L×0.5M_1 = 4L \times 0.5 M1=2L N⋅mM_1 = 2L \text{ N}\cdot\text{m}
      • Direction: Clockwise.
    • Moment from the Plank's Weight (7 N) (MWM_W):

      • Force: 7 N7 \text{ N}.
      • Distance from pivot: The weight acts at the center, L2\frac{L}{2} from the pivot.
      • Angle: The weight pulls straight down. If the plank is at an angle θ\theta to the horizontal, the perpendicular distance from the pivot to the line where the weight acts is L2cos⁡(θ)\frac{L}{2} \cos(\theta).
      • Calculation: MW=7 N×L2×cos⁡(θ)M_W = 7 \text{ N} \times \frac{L}{2} \times \cos(\theta) MW=3.5Lcos⁡(θ) N⋅mM_W = 3.5 L \cos(\theta) \text{ N}\cdot\text{m}
      • Direction: Clockwise.
    • Moment from the 8 N force (M2M_2):

      • Force: 8 N8 \text{ N}.
      • Distance from pivot: It's 34L\frac{3}{4}L from the pivot.
      • Angle: The force is 45∘45^\circ to the plank. The part of this force that causes rotation is 8sin⁡(45∘)8 \sin(45^\circ).
      • Calculation: M2=8 N×3L4×sin⁡(45∘)M_2 = 8 \text{ N} \times \frac{3L}{4} \times \sin(45^\circ) M2=6L×22M_2 = 6L \times \frac{\sqrt{2}}{2} M2=32L N⋅mM_2 = 3\sqrt{2} L \text{ N}\cdot\text{m}
      • Direction: Anti-clockwise.

  3. Set Up the Balance Equation

    For the plank to be balanced, the total clockwise moments must equal the total anti-clockwise moments:

    Total Clockwise Moments=Total Anti-clockwise Moments\text{Total Clockwise Moments} = \text{Total Anti-clockwise Moments} MW+M1=M2M_W + M_1 = M_2

    Substitute the expressions we found for each moment:

    3.5Lcos⁡(θ)+2L=32L3.5 L \cos(\theta) + 2L = 3\sqrt{2} L
  4. Solve for the Angle (θ\theta)

    • Notice that the length LL appears in every part of the equation. This is great because it means we can divide the entire equation by LL (since LL isn't zero), and it will cancel out! This means the exact length of the plank doesn't matter for finding the angle.

      3.5Lcos⁡(θ)L+2LL=32LL\frac{3.5 L \cos(\theta)}{L} + \frac{2L}{L} = \frac{3\sqrt{2} L}{L} 3.5cos⁡(θ)+2=323.5 \cos(\theta) + 2 = 3\sqrt{2}
    • Now, we want to get cos⁡(θ)\cos(\theta) by itself. First, subtract 2 from both sides:

      3.5cos⁡(θ)=32−23.5 \cos(\theta) = 3\sqrt{2} - 2
    • Let's calculate the value of 323\sqrt{2}:

      2≈1.4142\sqrt{2} \approx 1.4142 32≈3×1.4142=4.24263\sqrt{2} \approx 3 \times 1.4142 = 4.2426
    • Substitute this value back into the equation:

      3.5cos⁡(θ)=4.2426−23.5 \cos(\theta) = 4.2426 - 2 3.5cos⁡(θ)=2.24263.5 \cos(\theta) = 2.2426
    • Finally, divide by 3.5 to find cos⁡(θ)\cos(\theta):

      cos⁡(θ)=2.24263.5\cos(\theta) = \frac{2.2426}{3.5} cos⁡(θ)≈0.6407\cos(\theta) \approx 0.6407
    • To find the angle θ\theta itself, we use the inverse cosine function (often written as arccos⁡\arccos or cos⁡−1\cos^{-1}) on your calculator:

      θ=arccos⁡(0.6407)\theta = \arccos(0.6407) θ≈50.15∘\theta \approx 50.15^\circ

    So, when the plank is balanced, it makes an angle of about 50.15∘50.15^\circ with the horizontal ground.

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