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| <meta name="author" content="Aliaksandr Melnichenka"> | | <meta name="author" content="Aliaksandr Melnichenka"> |
| <meta name="date" content="2023-10" scheme="YYYY-MM"> | | <meta name="date" content="2023-10" scheme="YYYY-MM"> |
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| <meta property="og:description" content="The gun is fired at an angle \varphi to the horizon. Initial velocity of the projectile v. The ground surface is horizontal. Find: <br>a) the horizontal and vertical projections of velocity as a function of time; <br>b) the dependence of the x and y coordinates on time; <br>c) the trajectory equation, i.e. the dependence of y on x; <br>d) the flight time, the highest altitude and range of the projectile."> | | <meta property="og:description" content="The gun is fired at an angle \varphi to the horizon. Initial velocity of the projectile v. The ground surface is horizontal. Find: <br>a) the horizontal and vertical projections of velocity as a function of time; <br>b) the dependence of the x and y coordinates on time; <br>c) the trajectory equation, i.e. the dependence of y on x; <br>d) the flight time, the highest altitude and range of the projectile."> |
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| <title>The gun is fired at an angle \varphi to the horizon. Initial velocity of the projectile v. The ground surface is horizontal. Find: <br>a) the horizontal and vertical projections of velocity as a function of time; <br>b) the dependence of the x and y coordinates on time; <br>c) the trajectory equation, i.e. the dependence of y on x; <br>d) the flight time, the highest altitude and range of the projectile.</title> | | <title>The gun is fired at an angle \varphi to the horizon. Initial velocity of the projectile v. The ground surface is horizontal. Find: <br>a) the horizontal and vertical projections of velocity as a function of time; <br>b) the dependence of the x and y coordinates on time; <br>c) the trajectory equation, i.e. the dependence of y on x; <br>d) the flight time, the highest altitude and range of the projectile.</title> |
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| <h3> Statement </h3> | | <h3> Statement </h3> |
| <p> | | <p> |
| $1.3.6.$ The gun is fired at an angle $\varphi$ to the horizon. Initial velocity of the projectile $v.$ The ground surface is horizontal. Find: <br>a) the horizontal and vertical projections of velocity as a function of time; <br>b) the dependence of the $x$ and $y$ coordinates on time; <br>c) the trajectory equation, i.e. the dependence of $y$ on $x$; <br>d) the flight time, the highest altitude and range of the projectile. | | $1.3.6.$ The gun is fired at an angle $\varphi$ to the horizon. Initial velocity of the projectile $v.$ The ground surface is horizontal. Find: <br>a) the horizontal and vertical projections of velocity as a function of time; <br>b) the dependence of the $x$ and $y$ coordinates on time; <br>c) the trajectory equation, i.e. the dependence of $y$ on $x$; <br>d) the flight time, the highest altitude and range of the projectile. |
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| <h3>Solution</h3> | | <h3>Solution</h3> |
| <p> | | <p> |
| a) Since the external force (gravitational force) acts only in the vertical direction, the horizontal component of the velocity $v_x$ remains unchanged | | a) Since the external force (gravitational force) acts only in the vertical direction, the horizontal component of the velocity $v_x$ remains unchanged |
| $$ v_x = v \cdot \cos{\varphi}\;(1) $$ | | $$ v_x = v \cdot \cos{\varphi}\;(1) $$ |
| And the vertical component depends as a function of time | | And the vertical component depends as a function of time |
| $$ v_y(t) = v \cdot \sin{\varphi} - gt\;(2) $$ | | $$ v_y(t) = v \cdot \sin{\varphi} - gt\;(2) $$ |
| b) Based on the obtained expressions for the speed $(1)$ and $(2)$, we obtain the dependence of the horizontal and vertical coordinates on time, respectively: | | b) Based on the obtained expressions for the speed $(1)$ and $(2)$, we obtain the dependence of the horizontal and vertical coordinates on time, respectively: |
| $$ y(t) = vt \cdot \sin{\varphi} - \frac{gt^2}{2}\;(3) $$ | | $$ y(t) = vt \cdot \sin{\varphi} - \frac{gt^2}{2}\;(3) $$ |
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| $$ x(t) = vt \cdot \cos{\varphi}\;(4) $$ | | $$ x(t) = vt \cdot \cos{\varphi}\;(4) $$ |
| c) From $(4)$ we express $t$: | | c) From $(4)$ we express $t$: |
| $$ t = \frac{x}{v \cdot \cos{\varphi}} \;(5) $$ | | $$ t = \frac{x}{v \cdot \cos{\varphi}} \;(5) $$ |
| And we substitute in $(3)$ | | And we substitute in $(3)$ |
| $$ y(x) = x \tan \varphi-\frac{gx^2}{2v^2\cos^2\varphi}\;(6) $$ | | $$ y(x) = x \tan \varphi-\frac{gx^2}{2v^2\cos^2\varphi}\;(6) $$ |
| d) The maximum height is achieved when the velocity is directed horizontally $(v_y = 0)$: | | d) The maximum height is achieved when the velocity is directed horizontally $(v_y = 0)$: |
| $$ t_0 = \frac{v\sin\varphi}{g}\;(7) $$ | | $$ t_0 = \frac{v\sin\varphi}{g}\;(7) $$ |
| Substituting $(7)$ into $(3)$: | | Substituting $(7)$ into $(3)$: |
| $$ H = \frac{v^2}{2g}\operatorname{sin}^2\varphi\;(8) $$ | | $$ H = \frac{v^2}{2g}\operatorname{sin}^2\varphi\;(8) $$ |
| From the symmetry of the parabola, the time after which the body will again be on the ground$(y = 0)$, we find as: | | From the symmetry of the parabola, the time after which the body will again be on the ground$(y = 0)$, we find as: |
| $$ T = 2t_0 = \frac{2v\sin\varphi}{g}\;(9) $$ | | $$ T = 2t_0 = \frac{2v\sin\varphi}{g}\;(9) $$ |
| Substituting $(9)$ into $(4)$: | | Substituting $(9)$ into $(4)$: |
| $$ L=\frac{v^2}{g}\operatorname{sin}2\varphi\;(10) $$ | | $$ L=\frac{v^2}{g}\operatorname{sin}2\varphi\;(10) $$ |
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| <h4>Answer</h4> | | <h4>Answer</h4> |
| <p> | | <p> |
| a) $v_x= v\cos\varphi, v_y = v\sin\varphi-gt$<br> | | a) $v_x= v\cos\varphi, v_y = v\sin\varphi-gt$<br> |
| b) $x = (v\cos\varphi)t, y = (v\sin{\varphi})t - gt^2/2$<br> | | b) $x = (v\cos\varphi)t, y = (v\sin{\varphi})t - gt^2/2$<br> |
| c) $y = x \tan \varphi-\frac{gx^2}{2v^2\cos^2\varphi} =x\operatorname{tg}\varphi-\frac{gx^2}{2v^2}(\operatorname{tg}^2\varphi+1)$<br> | | c) $y = x \tan \varphi-\frac{gx^2}{2v^2\cos^2\varphi} =x\operatorname{tg}\varphi-\frac{gx^2}{2v^2}(\operatorname{tg}^2\varphi+1)$<br> |
| d) $T=\frac{2v}{g}\operatorname{sin}\varphi, H=\frac{v^2}{2g}\operatorname{sin}^2\varphi, L=\frac{v^2}{g}\operatorname{sin}2\varphi$<br> | | d) $T=\frac{2v}{g}\operatorname{sin}\varphi, H=\frac{v^2}{2g}\operatorname{sin}^2\varphi, L=\frac{v^2}{g}\operatorname{sin}2\varphi$<br> |
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