Learn how to solve projectile motion problems in physics with step-by-step solutions. This tutorial covers height, time, maximum height, and the time an object hits the ground. Perfect for high school and college students practicing physics and math problems.
If air resistance is ignored, the height \( h \) of a projectile above the ground after \( t \) seconds is given by
\[ h(t) = -\tfrac{1}{2} g t^{2} + V_{0} t + h_{0} \]where \( g \) is the acceleration due to gravity (approximately \( 32 \,\text{ft/s}^{2} \) on Earth), \( V_{0} \) is the initial velocity at \( t = 0 \), and \( h_{0} \) is the initial height at \( t = 0 \).
For an object that is dropped (initial velocity zero), the distance traveled is
\[ h(t) = \tfrac{1}{2} g t^2 \]For a quadratic function of the form
\[ h(t) = a t^2 + b t + c \]with a negative coefficient \( a \), the maximum height occurs at \[ t = - \dfrac{b}{2 a} \] which corresponds to the vertex of the parabola representing \( h(t) \).
The formula \[ h (t) = -16 t^2 + 32 t + 80 \] gives the height h above ground, in feet, of an object thrown, at \( t = 0 \), straight upward from the top of an \( 80 \) feet building.
A rock is dropped into a well and the distance traveled is \[ d = 16t^{2} \quad \text{(in feet),} \] where \(t\) is the time in seconds. If the water splash is heard \(3\) seconds after the rock was dropped, and the speed of sound is \(1100 \ \text{ft/sec},\) approximate the height of the well.
Let \(T_{1}\) be the time it takes the rock to reach the bottom of the well. If \(H\) is the height of the well, then \[ H = 16 T_{1}^{2}. \] Let \(T_{2}\) be the time it takes the sound wave to reach the top of the well. Then \[ H = 1100 T_{2}. \] The relationship between \(T_{1}\) and \(T_{2}\) is \[ T_{1} + T_{2} = 3. \] Eliminate \(H\) \[ 16 T_{1}^{2} = 1100 T_{2}. \] Substitute \(T_{2} = 3 - T_{1}\): \[ 16 T_{1}^{2} = 1100 (3 - T_{1}). \] Form the quadratic equation \[ 16 T_{1}^{2} + 1100 T_{1} - 3300 = 0. \] Solve for \(T_{1}\) The quadratic has two solutions, but only one is positive: \[ T_{1} \approx 2.88 \ \text{seconds}. \] Calculate the height of the well \[ H = 16 T_{1}^{2} = 16 (2.88)^{2} \approx 132.7 \ \text{feet}. \]
From the top of a building, an object is thrown upward with an initial speed of \(64 \, \text{ft/sec}\). It touches the ground \(5 \, \text{seconds}\) later. What is the height of the building?
The formula for the height \( h \) of a projectile thrown upward is given by \[ h(t) = -\tfrac{1}{2} g t^{2} + V_{0} t + H_{0} \] where \( g \) is a constant equal to \( 32 \). The initial speed \( V_{0} \) is known, and when \( t = 5 \) seconds the projectile touches the ground, i.e., \( h = 0 \). Here, \( H_{0} \) is the initial height (the height of the building). Thus, we can write \[ 0 = -\tfrac{1}{2}(32)(5)^{2} + (64)(5) + H_{0} \] Solving for \( H_{0} \), we get the initial height which is the height of the building. \[ H_{0} = 80 \ \text{feet} \]
From ground, an object is thrown upward with an initial speed \( V_0 \). Three seconds later, it reaches a maximum height. What is the initial velocity \( V_0 \)?
The height \( h \) of a projectile thrown upward from the ground (initial height \( H_0 = 0 \)) is given by \[ h(t) = -\tfrac{1}{2}(32)t^2 + V_0 t \] which simplifies to \[ h(t) = -16t^2 + V_0 t. \] The maximum height occurs at \[ t = \frac{-V_0}{2(-16)}. \] But this time is given to be \( 3 \) seconds. Hence \[ \frac{-V_0}{2(-16)} = 3. \] Solving for \( V_0 \), we obtain the initial velocity \[ V_0 = 96 \ \text{feet/second}. \]