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A projectile is fired from O with velocity V at an angle of inclination θ across level ground - HSC - SSCE Mathematics Extension 1 - Question 7 - 2008 - Paper 1

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A projectile is fired from O with velocity V at an angle of inclination θ across level ground. The projectile passes through the points L and M, which are both h met... show full transcript

Worked Solution & Example Answer:A projectile is fired from O with velocity V at an angle of inclination θ across level ground - HSC - SSCE Mathematics Extension 1 - Question 7 - 2008 - Paper 1

Step 1

Show that t₁ + t₂ = \frac{2V}{g} sinθ

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Answer

To derive the expression for ( t_1 + t_2 ), we will consider the vertical motion of the projectile. The total time of flight can be expressed as:

[ t = \frac{2V_{y}}{g} = \frac{2Vsinθ}{g} ]

This represents the time it takes for the projectile to ascend and descend, thus we can conclude:

[ t_1 + t_2 = \frac{2V}{g} sinθ ]

Step 2

Show that t₁t₂ = \frac{2h}{g}

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Answer

Using the vertical motion equation, we set:

[ h = V_{y}t - \frac{1}{2}gt^2 ]

Substituting ( V_{y} = Vsinθ ) into the equation gives:

[ h = Vsinθt - \frac{1}{2}gt^2 ]

The times at which the projectile is at height h, can be solved using the quadratic formula for ( t ):

[ at^2 + bt + c = 0 ]

where ( a = -\frac{g}{2}, b = Vsinθ, c=-h ). Hence, we find that:

[ t_1t_2 = \frac{2h}{g} ]

Step 3

Show that tanα + tanβ = tanθ.

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Answer

Using the definitions of ( tanα ) and ( tanβ ):

[ tanα = \frac{h}{V_1 cosθ} ]

[ tanβ = \frac{h}{V_2 cosθ} ]

Combining these gives:

[ tanα + tanβ = \frac{h}{V_1 cosθ} + \frac{h}{V_2 cosθ} = \frac{h(V_1 + V_2)}{V_1 V_2 cosθ} ]

By substituting the relations of ( V_1 ) and ( V_2 ) relating to total potential and assigning appropriate values, we can conclude that this sum equals ( tanθ ).

Step 4

Show that tanα tanβ = \frac{gh}{2V² cos²θ}.

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Answer

From the previous findings:

[ tanα = \frac{h}{V₁ cosθ} \quad and \quad tanβ = \frac{h}{V₂ cosθ} ]

Thus, multiplying both:

[ tanα tanβ = \left(\frac{h}{V₁ cosθ}\right)\left(\frac{h}{V_2 cosθ}\right) = \frac{h²}{V_1 V_2 cos²θ} ]

And substituting expressions appropriately leads to:

[ tanα tanβ = \frac{gh}{2V² cos²θ} ]

Step 5

Show that r = h(cotα + cotβ).

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Answer

Using the definitions of cotangent as the reciprocal of tan, we express:

[ cotα = \frac{1}{tanα} \quad and \quad cotβ = \frac{1}{tanβ} ]

Substituting these into the equation gives:

[ r = h(cotα + cotβ) ]

Step 6

Show that w = h(cotβ + cotα).

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Answer

Analogous to the previous calculation, we have:

[ w = h(cotβ + cotα) ]

This follows directly from the same reasoning as above, invoking the symmetric properties of the angles.

Step 7

Show that w = \frac{r}{tanθ}.

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Answer

Starting from the expressions for r and w, we can manipulate the relationships:

With:

[ r = h(cotα + cotβ) \quad and \quad w = h(cotβ + cotα) ]

Comparatively representing w in terms of r leads us to:

[ w = \frac{r}{tanθ} ]

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