A velocity-time (v-t) graph for constant acceleration is always a straight line because the rate of change of velocity is uniform.
Deriving : The gradient of a velocity-time graph represents acceleration. By calculating the gradient as , we get , which rearranges to the first equation.
Deriving : The area under a velocity-time graph represents displacement. For a constant acceleration graph, this area forms a trapezium with parallel sides of lengths and and a height of .
Deriving : This is found by splitting the area under the graph into a rectangle (area ) and a triangle (area ). Substituting into the triangle area yields the final form.
Since acceleration is the derivative of velocity with respect to time (), velocity can be derived by integrating acceleration: .
By applying the initial condition that at , velocity , we find that the constant of integration , resulting in .
Similarly, displacement is the integral of velocity: .
Given that at , displacement (relative to the start), the constant becomes , yielding the standard displacement formula.
The equation is derived by eliminating the time variable () from the other equations.
By rearranging to and substituting this into , we obtain .
Expanding the numerator (a difference of two squares) gives , which rearranges to the final squared velocity formula.
Check the Units: Always ensure that is in , and in , and in before attempting a derivation or calculation.
Directional Consistency: When deriving or using these formulas, define a positive direction (e.g., upwards or to the right) and stick to it for and .
Identify the 'Missing' Variable: Each of the five equations lacks exactly one of the five variables. In exams, identify which variable is not mentioned and choose the formula that excludes it.
Verification: If asked to derive , remember to explicitly state that the area under the v-t graph is being calculated.