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A particle is projected from a point O on horizontal ground with an initial speed U m/s at an angle θ to the horizontal. It passes through the point (40,10). Given that tan θ = 3/4, find U, velocity c

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Here is the solution to the projectile motion problem:

Question 3:
A particle is projected from a point O on horizontal ground with an initial speed UU m/s at an angle θ\theta to the horizontal. It passes through the point (40,10)(40,10). Given that tan⁡θ=3/4\tan \theta = 3/4, find:

a) The value of UU.

b) The horizontal and the vertical components of the velocity when t=2t = 2 s. State, with a reason, whether the particle is rising or falling at this instance.

c) The total time for which the particle is at a height greater than 5 m.
(take g=10 m/s2g=10 \text{ m/s}^2)

First, let's determine sin⁡θ\sin \theta and cos⁡θ\cos \theta from tan⁡θ=3/4\tan \theta = 3/4.
Using a right-angled triangle with opposite side 3 and adjacent side 4, the hypotenuse is 32+42=9+16=25=5\sqrt{3^2+4^2} = \sqrt{9+16} = \sqrt{25} = 5.
So, sin⁡θ=35\sin \theta = \frac{3}{5} and cos⁡θ=45\cos \theta = \frac{4}{5}.

The equations of motion for a projectile are:
Horizontal displacement: x=(Ucos⁡θ)tx = (U \cos \theta) t
Vertical displacement: y=(Usin⁡θ)t−12gt2y = (U \sin \theta) t - \frac{1}{2} g t^2

a) The value of UU.
The particle passes through the point (x,y)=(40,10)(x,y) = (40,10).
Substitute x=40x=40, y=10y=10, cos⁡θ=4/5\cos \theta = 4/5, sin⁡θ=3/5\sin \theta = 3/5, and g=10 m/s2g=10 \text{ m/s}^2 into the equations:

  1. Use the horizontal displacement equation.

    40=(U⋅45)t40 = \left(U \cdot \frac{4}{5}\right) t 40=4U5t40 = \frac{4U}{5} t 200=4Ut200 = 4Ut Ut=50(1)Ut = 50 \quad (1)
  2. Use the vertical displacement equation.

    10=(U⋅35)t−12(10)t210 = \left(U \cdot \frac{3}{5}\right) t - \frac{1}{2} (10) t^2 10=3U5t−5t2(2)10 = \frac{3U}{5} t - 5t^2 \quad (2)
  3. Substitute Ut=50Ut=50 from (1) into (2).

    10=35(50)−5t210 = \frac{3}{5} (50) - 5t^2 10=3×10−5t210 = 3 \times 10 - 5t^2 10=30−5t210 = 30 - 5t^2 5t2=30−105t^2 = 30 - 10 5t2=205t^2 = 20 t2=4t^2 = 4 t=2 s(since t>0)t = 2 \text{ s} \quad (\text{since } t > 0)
  4. Substitute t=2t=2 s back into equation (1) to find UU.

    U(2)=50U(2) = 50 U=502U = \frac{50}{2} U=25 m/sU = 25 \text{ m/s}

    The value of UU is 25 m/s\boxed{\text{25 m/s}}.

    b) The horizontal and the vertical components of the velocity when t=2t = 2 s. State, with a reason, whether the particle is rising or falling at this instance.
    The velocity components are given by:
    Horizontal velocity: vx=Ucos⁡θv_x = U \cos \theta
    Vertical velocity: vy=Usin⁡θ−gtv_y = U \sin \theta - gt

  5. Calculate the horizontal velocity component at t=2t=2 s.

    vx=25⋅45v_x = 25 \cdot \frac{4}{5} vx=5×4v_x = 5 \times 4 vx=20 m/sv_x = 20 \text{ m/s}
  6. Calculate the vertical velocity component at t=2t=2 s.

    vy=25⋅35−(10)(2)v_y = 25 \cdot \frac{3}{5} - (10)(2) vy=5×3−20v_y = 5 \times 3 - 20 vy=15−20v_y = 15 - 20 vy=−5 m/sv_y = -5 \text{ m/s}
  7. Determine if the particle is rising or falling.

    Since the vertical component of velocity vy=−5 m/sv_y = -5 \text{ m/s} is negative, the particle is moving downwards.
    The horizontal component of velocity is 20 m/s\boxed{\text{20 m/s}}.
    The vertical component of velocity is *−5m/s∗\boxed{\text*{-5 m/s*}}.
    The particle is falling because its vertical velocity component is negative.

    c) The total time for which the particle is at a height greater than 5 m.
    We need to find the times when y=5y=5 m and then calculate the duration between these times.
    Using the vertical displacement equation: y=(Usin⁡θ)t−12gt2y = (U \sin \theta) t - \frac{1}{2} g t^2
    Substitute y=5y=5, U=25U=25, sin⁡θ=3/5\sin \theta = 3/5, and g=10g=10:

    5=(25⋅35)t−12(10)t25 = \left(25 \cdot \frac{3}{5}\right) t - \frac{1}{2} (10) t^2 5=(5×3)t−5t25 = (5 \times 3) t - 5t^2 5=15t−5t25 = 15t - 5t^2
  8. Rearrange the equation into a quadratic form.

    5t2−15t+5=05t^2 - 15t + 5 = 0

    Divide by 5:

    t2−3t+1=0t^2 - 3t + 1 = 0
  9. Solve the quadratic equation for tt using the quadratic formula t=−b±b2−4ac2at = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}.

    Here, a=1a=1, b=−3b=-3, c=1c=1.

    t=−(−3)±(−3)2−4(1)(1)2(1)t = \frac{-(-3) \pm \sqrt{(-3)^2 - 4(1)(1)}}{2(1)} t=3±9−42t = \frac{3 \pm \sqrt{9 - 4}}{2} t=3±52t = \frac{3 \pm \sqrt{5}}{2}

    The two times when the particle is at a height of 5 m are:

    t1=3−52 st_1 = \frac{3 - \sqrt{5}}{2} \text{ s} t2=3+52 st_2 = \frac{3 + \sqrt{5}}{2} \text{ s}
  10. Calculate the total time for which the particle is at a height greater than 5 m.

    This is the difference between t2t_2 and t1t_1.

    Total time=t2−t1=(3+52)−(3−52)\text{Total time} = t_2 - t_1 = \left(\frac{3 + \sqrt{5}}{2}\right) - \left(\frac{3 - \sqrt{5}}{2}\right) Total time=3+5−3+52\text{Total time} = \frac{3 + \sqrt{5} - 3 + \sqrt{5}}{2} Total time=252\text{Total time} = \frac{2\sqrt{5}}{2} Total time=5 s\text{Total time} = \sqrt{5} \text{ s}

    The total time for which the particle is at a height greater than 5 m is 5 s\boxed{\text{}\sqrt{5}\text{ s}}.

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