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Physics - SSS 2 Third Term Examination. Answer Question One and any Other Three (3). 1. A simple pendulum for 20 oscillations.

Physics

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Question 3(c): Calculate the reactions at P and Q.

  • Step 1: Identify forces and positions. Let the left end of the bar be the origin (x=0x=0). The total length of the bar is 3m+2m+3m+2m=10m3\text{m} + 2\text{m} + 3\text{m} + 2\text{m} = 10\text{m}. The weight of the uniform bar, F2=20NF_2 = 20\text{N}, acts at its center, which is at x=10m/2=5mx = 10\text{m}/2 = 5\text{m}. The supports are at P (reaction RPR_P) and Q (reaction RQR_Q). From the diagram: Position of P: xP=0mx_P = 0\text{m} (assuming P is at the left end) Position of F1=15NF_1 = 15\text{N}: xF1=3mx_{F_1} = 3\text{m} Position of F2=20NF_2 = 20\text{N}: xF2=5mx_{F_2} = 5\text{m} Position of Q: xQ=5m+3m=8mx_Q = 5\text{m} + 3\text{m} = 8\text{m} Position of F3=5NF_3 = 5\text{N}: xF3=8m+2m=10mx_{F_3} = 8\text{m} + 2\text{m} = 10\text{m}

  • Step 2: Apply the first condition for equilibrium (sum of vertical forces is zero). Assuming upward forces are positive:

    ∑Fy=0\sum F_y = 0 RP+RQ−F1−F2−F3=0R_P + R_Q - F_1 - F_2 - F_3 = 0 RP+RQ−15N−20N−5N=0R_P + R_Q - 15\text{N} - 20\text{N} - 5\text{N} = 0 RP+RQ=40N(Equation 1)R_P + R_Q = 40\text{N} \quad (\text{Equation 1})
  • Step 3: Apply the second condition for equilibrium (sum of moments about a point is zero). Take moments about point P (x=0x=0). Clockwise moments are negative, anti-clockwise moments are positive.

    ∑MP=0\sum M_P = 0 (RQ×8m)−(F1×3m)−(F2×5m)−(F3×10m)=0(R_Q \times 8\text{m}) - (F_1 \times 3\text{m}) - (F_2 \times 5\text{m}) - (F_3 \times 10\text{m}) = 0 (RQ×8)−(15×3)−(20×5)−(5×10)=0(R_Q \times 8) - (15 \times 3) - (20 \times 5) - (5 \times 10) = 0 8RQ−45−100−50=08R_Q - 45 - 100 - 50 = 0 8RQ−195=08R_Q - 195 = 0 8RQ=1958R_Q = 195 RQ=1958R_Q = \frac{195}{8} RQ=24.375NR_Q = 24.375\text{N}
  • Step 4: Calculate RPR_P using Equation 1.

    RP+RQ=40NR_P + R_Q = 40\text{N} RP+24.375N=40NR_P + 24.375\text{N} = 40\text{N} RP=40N−24.375NR_P = 40\text{N} - 24.375\text{N} RP=15.625NR_P = 15.625\text{N}
  • Step 5: Verify by taking moments about Q (x=8mx=8\text{m}). Anti-clockwise moments are positive, clockwise moments are negative.

    ∑MQ=0\sum M_Q = 0 (RP×8m)+(F1×(8−3)m)+(F2×(8−5)m)−(F3×(10−8)m)=0(R_P \times 8\text{m}) + (F_1 \times (8-3)\text{m}) + (F_2 \times (8-5)\text{m}) - (F_3 \times (10-8)\text{m}) = 0 (RP×8)+(15×5)+(20×3)−(5×2)=0(R_P \times 8) + (15 \times 5) + (20 \times 3) - (5 \times 2) = 0 8RP+75+60−10=08R_P + 75 + 60 - 10 = 0 8RP+135−10=08R_P + 135 - 10 = 0 8RP+125=08R_P + 125 = 0 8RP=−1258R_P = -125 RP=−1258R_P = -\frac{125}{8} RP=−15.625NR_P = -15.625\text{N}

    The negative sign for RPR_P indicates that the force at P would need to be acting downwards to maintain equilibrium, or the bar would lift off the support at P. However, since the question asks for the reaction force, we provide the calculated value.

The reactions at P and Q are:

RP=−15.625N\boxed{R_P = -15.625\text{N}} RQ=24.375N\boxed{R_Q = 24.375\text{N}}

Question 2(c): SHM Calculation
Given displacement y=rsin⁡(wt+0.8)y = r \sin(wt+0.8).
Initial displacement (t=0t=0): y0=3.5y_0 = 3.5.
Initial velocity (t=0t=0): v0=5.6 ms−1v_0 = 5.6 \text{ ms}^{-1}.

  • Step 1: Calculate rr (amplitude). At t=0t=0, the displacement is y0=rsin⁡(w⋅0+0.8)=rsin⁡(0.8)y_0 = r \sin(w \cdot 0 + 0.8) = r \sin(0.8). Given y0=3.5y_0 = 3.5:

    3.5=rsin⁡(0.8)3.5 = r \sin(0.8)

    Using a calculator, sin⁡(0.8 radians)≈0.717356\sin(0.8 \text{ radians}) \approx 0.717356.

    r=3.50.717356r = \frac{3.5}{0.717356} r≈4.879 mr \approx 4.879 \text{ m}
  • Step 2: Calculate ww (angular frequency). First, find the velocity equation by differentiating the displacement equation with respect to time:

    v=dydt=ddt[rsin⁡(wt+0.8)]=rwcos⁡(wt+0.8)v = \frac{dy}{dt} = \frac{d}{dt} [r \sin(wt+0.8)] = rw \cos(wt+0.8)

    At t=0t=0, the velocity is v0=rwcos⁡(w⋅0+0.8)=rwcos⁡(0.8)v_0 = rw \cos(w \cdot 0 + 0.8) = rw \cos(0.8). Given v0=5.6 ms−1v_0 = 5.6 \text{ ms}^{-1}:

    5.6=rwcos⁡(0.8)5.6 = rw \cos(0.8)

    We know r≈4.879r \approx 4.879 and cos⁡(0.8 radians)≈0.696706\cos(0.8 \text{ radians}) \approx 0.696706.

    5.6=(4.879)⋅w⋅(0.696706)5.6 = (4.879) \cdot w \cdot (0.696706) 5.6=3.399⋅w5.6 = 3.399 \cdot w w=5.63.399w = \frac{5.6}{3.399} w≈1.647 rad/sw \approx 1.647 \text{ rad/s}
  • Step 3: Calculate TT (period). The period TT is related to the angular frequency ww by the formula T=2πwT = \frac{2\pi}{w}.

    T=2π1.647T = \frac{2\pi}{1.647} T≈2×3.141591.647T \approx \frac{2 \times 3.14159}{1.647} T≈3.815 sT \approx 3.815 \text{ s}
  • Step 4: Calculate velocity at t=1.42 sect = 1.42 \text{ sec}. Using the velocity equation v=rwcos⁡(wt+0.8)v = rw \cos(wt+0.8):

    v=(4.879)⋅(1.647)⋅cos⁡((1.647⋅1.42)+0.8)v = (4.879) \cdot (1.647) \cdot \cos((1.647 \cdot 1.42) + 0.8) v=8.036⋅cos⁡(2.33874+0.8)v = 8.036 \cdot \cos(2.33874 + 0.8) v=8.036⋅cos⁡(3.13874)v = 8.036 \cdot \cos(3.13874)

    Using a calculator, cos⁡(3.13874 radians)≈−0.99999\cos(3.13874 \text{ radians}) \approx -0.99999.

    v=8.036⋅(−0.99999)v = 8.036 \cdot (-0.99999) v≈−8.036 ms−1v \approx -8.036 \text{ ms}^{-1}

The calculated values are:

  • (i) r≈4.879 mr \approx \boxed{4.879\text{ m}}, w≈1.647 rad/sw \approx \boxed{1.647\text{ rad/s}}, T≈3.815 sT \approx \boxed{3.815\text{ s}}
  • (ii) Velocity at t=1.42 sec≈−8.036 ms−1t=1.42\text{ sec} \approx \boxed{-8.036\text{ ms}^{-1}}
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