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An archer fires an arrow at an angle of 40° above the horizontal with an initial speed of 98 m/sec. The height of the archer is 171.5 cm. Find the horizontal distance the arrow travels before it hits the ground.

967.15 m

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One final question remains: In general, what is the maximum distance a projectile can travel, given its initial speed? To determine this distance, we assume the projectile is fired from ground level and we wish it to return to ground level. In other words, we want to determine an equation for the range. In this case, the equation of projectile motion is

s ( t ) = v 0 t cos θ i + ( v 0 t sin θ 1 2 g t 2 ) j .

Setting the second component equal to zero and solving for t yields

v 0 t sin θ 1 2 g t 2 = 0 t ( v 0 sin θ 1 2 g t ) = 0.

Therefore, either t = 0 or t = 2 v 0 sin θ g . We are interested in the second value of t , so we substitute this into s ( t ) , which gives

s ( 2 v 0 sin θ g ) = v 0 ( 2 v 0 sin θ g ) cos θ i + ( v 0 ( 2 v 0 sin θ g ) sin θ 1 2 g ( 2 v 0 sin θ g ) 2 ) j = ( 2 v 0 2 sin θ cos θ g ) i = v 0 2 sin 2 θ g i .

Thus, the expression for the range of a projectile fired at an angle θ is

R = v 0 2 sin 2 θ g i .

The only variable in this expression is θ . To maximize the distance traveled, take the derivative of the coefficient of i with respect to θ and set it equal to zero:

d d θ ( v 0 2 sin 2 θ g ) = 0 2 v 0 2 cos 2 θ g = 0 θ = 45 ° .

This value of θ is the smallest positive value that makes the derivative equal to zero. Therefore, in the absence of air resistance, the best angle to fire a projectile (to maximize the range) is at a 45 ° angle. The distance it travels is given by

s ( 2 v 0 sin 45 g ) = v 0 2 sin 90 g i = v 0 2 g j .

Therefore, the range for an angle of 45 ° is v 0 2 / g .

Kepler’s laws

During the early 1600s, Johannes Kepler was able to use the amazingly accurate data from his mentor Tycho Brahe to formulate his three laws of planetary motion, now known as Kepler’s laws of planetary motion    . These laws also apply to other objects in the solar system in orbit around the Sun, such as comets (e.g., Halley’s comet) and asteroids. Variations of these laws apply to satellites in orbit around Earth.

Kepler’s laws of planetary motion

  1. The path of any planet about the Sun is elliptical in shape, with the center of the Sun located at one focus of the ellipse (the law of ellipses).
  2. A line drawn from the center of the Sun to the center of a planet sweeps out equal areas in equal time intervals (the law of equal areas) ( [link] ).
  3. The ratio of the squares of the periods of any two planets is equal to the ratio of the cubes of the lengths of their semimajor orbital axes (the law of harmonies).
This figure is an elliptical curve labeled “planets orbit”. The sun is represented towards the left inside the ellipse, at a focal point. Along the ellipse there are points A,B,C,D,E,F. There are line segments from the sun to each point.
Kepler’s first and second laws are pictured here. The Sun is located at a focus of the elliptical orbit of any planet. Furthermore, the shaded areas are all equal, assuming that the amount of time measured as the planet moves is the same for each region.

Kepler’s third law is especially useful when using appropriate units. In particular, 1 astronomical unit is defined to be the average distance from Earth to the Sun, and is now recognized to be 149,597,870,700 m or, approximately 93,000,000 mi. We therefore write 1 A.U. = 93,000,000 mi. Since the time it takes for Earth to orbit the Sun is 1 year, we use Earth years for units of time. Then, substituting 1 year for the period of Earth and 1 A.U. for the average distance to the Sun, Kepler’s third law can be written as

Practice Key Terms 6

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Source:  OpenStax, Calculus volume 3. OpenStax CNX. Feb 05, 2016 Download for free at http://legacy.cnx.org/content/col11966/1.2
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