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Define the following terms: Resultant force Elastic limit Strain Hydrostatic pressure Second moment of area

Physics

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here are the solutions for Question 1, Question 2, and Question 3.

SECTION A: QUESTION 1: GENERAL

1.1 Resultant force

The resultant force is the single force that produces the same effect on a body as all the individual forces acting on it. It is the vector sum of all forces.

1.2 Elastic limit

The elastic limit is the maximum stress that a material can withstand without undergoing permanent deformation. If the stress exceeds this limit, the material will not return to its original shape once the stress is removed.

1.3 Strain

Strain is a measure of the deformation of a material, defined as the ratio of the change in dimension (e.g., length, volume) to the original dimension. It is a dimensionless quantity.

1.4 Hydrostatic pressure

Hydrostatic pressure is the pressure exerted by a fluid at rest due to the force of gravity. It increases with depth and is calculated as P=ρghP = \rho gh, where ρ\rho is the fluid density, gg is the acceleration due to gravity, and hh is the depth.

1.5 Second moment of area

The second moment of area, also known as the area moment of inertia, is a geometrical property of a cross-section that describes how its area is distributed with respect to an axis. It is crucial in beam bending calculations to determine a beam's resistance to bending and deflection.

SECTION B: QUESTION 2: KINEMATICS

2.1 A delivery truck travels at a velocity of 90 km/h90 \text{ km/h} on a bearing of 045∘045^\circ true. It has to deliver goods to a warehouse that is 120 km120 \text{ km} due East of its current position. A cross wind of 20 km/h20 \text{ km/h} from the South acts on the truck.

2.1.1 Determine the true course the driver must steer to reach the warehouse.

Let VTAV_{TA} be the velocity of the truck relative to the air (what the driver steers), with magnitude 90 km/h90 \text{ km/h} and unknown bearing θ\theta.
Let VWV_W be the velocity of the wind. Since it's from the South, it blows North, so VW=(0,20) km/hV_W = (0, 20) \text{ km/h}.
Let VGV_G be the resultant velocity of the truck relative to the ground. Since the destination is due East, VGV_G must be purely in the East direction, so VG=(VG,0)V_G = (V_G, 0).

The vector equation is VG=VTA+VWV_G = V_{TA} + V_W.
In components, using standard Cartesian coordinates (East as positive x, North as positive y):
VTA,x=90sin⁡θV_{TA,x} = 90 \sin\theta (East component, using bearing from North)
VTA,y=90cos⁡θV_{TA,y} = 90 \cos\theta (North component, using bearing from North)

  1. Set up the vector equation in components.

    (VG,0)=(90sin⁡θ,90cos⁡θ)+(0,20)(V_G, 0) = (90 \sin\theta, 90 \cos\theta) + (0, 20) (VG,0)=(90sin⁡θ,90cos⁡θ+20)(V_G, 0) = (90 \sin\theta, 90 \cos\theta + 20)
  2. Equate the y-components to find the steering angle θ\theta.

    0=90cos⁡θ+200 = 90 \cos\theta + 20 90cos⁡θ=−2090 \cos\theta = -20 cos⁡θ=−2090=−29\cos\theta = -\frac{20}{90} = -\frac{2}{9} θ=arccos⁡(−29)\theta = \arccos\left(-\frac{2}{9}\right) θ≈102.84∘\theta \approx \boxed{\text{102.84}^\circ}

    The driver must steer on a true course (bearing) of 102.84∘102.84^\circ.

    2.1.2 Calculate how long the journey will take.
  3. Calculate the magnitude of the resultant velocity VGV_G (the effective speed towards East).

    From the x-components:

    VG=90sin⁡θV_G = 90 \sin\theta

    Substitute θ≈102.84∘\theta \approx 102.84^\circ:

    VG=90sin⁡(102.84∘) km/hV_G = 90 \sin(102.84^\circ) \text{ km/h} VG≈90×0.975 km/hV_G \approx 90 \times 0.975 \text{ km/h} VG≈87.75 km/hV_G \approx 87.75 \text{ km/h}
  4. Calculate the time taken for the journey.

    The distance to the warehouse is D=120 kmD = 120 \text{ km} (East).

    t=DVGt = \frac{D}{V_G} t=120 km87.75 km/ht = \frac{120 \text{ km}}{87.75 \text{ km/h}} t≈1.3676 hourst \approx 1.3676 \text{ hours} t≈1 hour and (0.3676×60) minutest \approx 1 \text{ hour and } (0.3676 \times 60) \text{ minutes} t≈1 hour and 22.06 minutest \approx \boxed{\text{1 hour and 22.06 minutes}}

    2.2 A steel ball is projected from the top of a building 48 m48 \text{ m} high with an initial velocity of 18 m/s18 \text{ m/s} at an angle of 25∘25^\circ above the horizontal.

    Given:
    Initial velocity u=18 m/su = 18 \text{ m/s}
    Angle of projection α=25∘\alpha = 25^\circ
    Height of building H=48 mH = 48 \text{ m}
    Acceleration due to gravity g=9.81 m/s2g = 9.81 \text{ m/s}^2 (downwards)

    2.2.1 The maximum height above the ground reached by the ball.
  5. Resolve initial velocity into vertical component.

    uy=usin⁡α=18sin⁡(25∘) m/su_y = u \sin\alpha = 18 \sin(25^\circ) \text{ m/s} uy≈18×0.4226≈7.607 m/su_y \approx 18 \times 0.4226 \approx 7.607 \text{ m/s}
  6. Calculate the maximum height reached above the launch point (hmaxh_{max}).

    At maximum height, the vertical velocity vy=0v_y = 0.
    Using the kinematic equation vy2=uy2+2ghmaxv_y^2 = u_y^2 + 2gh_{max}:

    02=(7.607 m/s)2+2(−9.81 m/s2)hmax0^2 = (7.607 \text{ m/s})^2 + 2(-9.81 \text{ m/s}^2)h_{max} 0=57.866−19.62hmax0 = 57.866 - 19.62 h_{max} 19.62hmax=57.86619.62 h_{max} = 57.866 hmax=57.86619.62≈2.949 mh_{max} = \frac{57.866}{19.62} \approx 2.949 \text{ m}
  7. Calculate the maximum height above the ground.

    Total maximum height=H+hmax=48 m+2.949 m=50.95 m\text{Total maximum height} = H + h_{max} = 48 \text{ m} + 2.949 \text{ m} = \boxed{\text{50.95 m}}
    2.2.2 The horizontal distance from the foot of the building where the ball hits the ground.
    2.2.3 The time taken for the ball to hit the ground.
  8. Calculate the time taken for the ball to hit the ground.

    The total vertical displacement from the launch point to the ground is Δy=−48 m\Delta y = -48 \text{ m}.
    Using the kinematic equation Δy=uyt+12gt2\Delta y = u_y t + \frac{1}{2}gt^2:

    −48=(7.607)t+12(−9.81)t2-48 = (7.607)t + \frac{1}{2}(-9.81)t^2 −48=7.607t−4.905t2-48 = 7.607t - 4.905t^2

    Rearrange into a quadratic equation:

    4.905t2−7.607t−48=04.905t^2 - 7.607t - 48 = 0

    Using the quadratic formula t=−b±b2−4ac2at = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}:

    t=−(−7.607)±(−7.607)2−4(4.905)(−48)2(4.905)t = \frac{-(-7.607) \pm \sqrt{(-7.607)^2 - 4(4.905)(-48)}}{2(4.905)} t=7.607±57.866+941.769.81t = \frac{7.607 \pm \sqrt{57.866 + 941.76}}{9.81} t=7.607±999.6269.81t = \frac{7.607 \pm \sqrt{999.626}}{9.81} t=7.607±31.6179.81t = \frac{7.607 \pm 31.617}{9.81}

    Since time cannot be negative, we take the positive root:

    t=7.607+31.6179.81=39.2249.81≈3.998 st = \frac{7.607 + 31.617}{9.81} = \frac{39.224}{9.81} \approx \boxed{\text{3.998 s}}
  9. Calculate the horizontal distance.

    The horizontal velocity uxu_x is constant.

    ux=ucos⁡α=18cos⁡(25∘) m/su_x = u \cos\alpha = 18 \cos(25^\circ) \text{ m/s} ux≈18×0.9063≈16.313 m/su_x \approx 18 \times 0.9063 \approx 16.313 \text{ m/s}

    Horizontal distance x=uxtx = u_x t:

    x=16.313 m/s×3.998 sx = 16.313 \text{ m/s} \times 3.998 \text{ s} x≈65.22 mx \approx \boxed{\text{65.22 m}}

    2.3 A train accelerates uniformly from rest to a speed of 72 km/h72 \text{ km/h} in 45 seconds45 \text{ seconds}. It then travels at this constant speed for 3 minutes3 \text{ minutes} before applying the brakes and coming to rest uniformly in 60 seconds60 \text{ seconds}.

    2.3.1 Calculate the acceleration of the train.

    This refers to the first phase of motion.
    Initial velocity u1=0 m/su_1 = 0 \text{ m/s} (from rest)
    Final velocity v1=72 km/hv_1 = 72 \text{ km/h}
    Convert v1v_1 to m/s:

    v1=72 km/h×1000 m1 km×1 h3600 s=20 m/sv_1 = 72 \text{ km/h} \times \frac{1000 \text{ m}}{1 \text{ km}} \times \frac{1 \text{ h}}{3600 \text{ s}} = 20 \text{ m/s}

    Time t1=45 st_1 = 45 \text{ s}

  10. Calculate the acceleration a1a_1.

    a1=v1−u1t1a_1 = \frac{v_1 - u_1}{t_1} a1=20 m/s−0 m/s45 sa_1 = \frac{20 \text{ m/s} - 0 \text{ m/s}}{45 \text{ s}} a1=2045 m/s2=49 m/s2≈0.444 m/s2a_1 = \frac{20}{45} \text{ m/s}^2 = \frac{4}{9} \text{ m/s}^2 \approx \boxed{\text{0.444 m/s}^2}
    2.3.2 Determine the total distance travelled by the train from the start until it comes to rest.

    This involves three phases of motion:

    Phase 1: Acceleration
    Initial velocity u1=0 m/su_1 = 0 \text{ m/s}
    Final velocity v1=20 m/sv_1 = 20 \text{ m/s}
    Time t1=45 st_1 = 45 \text{ s}

  11. Calculate distance s1s_1.

    s1=(u1+v12)t1s_1 = \left(\frac{u_1 + v_1}{2}\right)t_1 s1=(0+202)×45=10×45=450 ms_1 = \left(\frac{0 + 20}{2}\right) \times 45 = 10 \times 45 = 450 \text{ m}

    Phase 2: Constant speed
    Speed v2=20 m/sv_2 = 20 \text{ m/s}
    Time t2=3 minutes=3×60 s=180 st_2 = 3 \text{ minutes} = 3 \times 60 \text{ s} = 180 \text{ s}

  12. Calculate distance s2s_2.

    s2=v2t2s_2 = v_2 t_2 s2=20 m/s×180 s=3600 ms_2 = 20 \text{ m/s} \times 180 \text{ s} = 3600 \text{ m}

    Phase 3: Deceleration
    Initial velocity u3=20 m/su_3 = 20 \text{ m/s}
    Final velocity v3=0 m/sv_3 = 0 \text{ m/s} (comes to rest)
    Time t3=60 st_3 = 60 \text{ s}

  13. Calculate distance s3s_3.

    s3=(u3+v32)t3s_3 = \left(\frac{u_3 + v_3}{2}\right)t_3 s3=(20+02)×60=10×60=600 ms_3 = \left(\frac{20 + 0}{2}\right) \times 60 = 10 \times 60 = 600 \text{ m}
  14. Calculate the total distance travelled.

    Stotal=s1+s2+s3S_{total} = s_1 + s_2 + s_3 Stotal=450 m+3600 m+600 m=4650 mS_{total} = 450 \text{ m} + 3600 \text{ m} + 600 \text{ m} = \boxed{\text{4650 m}}
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