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Da Nang-05/2015 Natural Science Department – Duy Tan University SPRING MOTION MODEL with Differential Equations In this section, we will learn: How to represent some mathematical models in the form of differential equations.
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We consider the motion of an object with mass m at the end of a vertical spring. MODEL FOR MOTION OF A SPRING
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If the spring is stretched (or compressed) x units from its natural length, it exerts a force proportional to x: restoring force = -kx where k is a positive constant (the spring constant). MODEL FOR MOTION OF A SPRING
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If we ignore any external resisting forces (due to air resistance or friction) then, by Newton’s Second Law, we have: SPRING MOTION MODEL Equation 3
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This is an example of a second-order differential equation. It involves second derivatives. SECOND-ORDER DIFFERENTIAL EQUATION
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SPRING MOTION MODEL Let’s see what we can guess about the form of the solution directly from the equation.
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We can rewrite Equation 3 in the form This says that the second derivative of x is proportional to x but has the opposite sign. SPRING MOTION MODEL
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We know two functions with this property, the sine and cosine functions. It turns out that all solutions of Equation 3 can be written as combinations of certain sine and cosine functions. SPRING MOTION MODEL
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This is not surprising. We expect the spring to oscillate about its equilibrium position. So, it is natural to think that trigonometric functions are involved. SPRING MOTION MODEL
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In general, a differential equation is an equation that contains an unknown function and one or more of its derivatives. GENERAL DIFFERENTIAL EQUATIONS
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ORDER The order of a differential equation is the order of the highest derivative that occurs in the equation.
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In all three equations, the independent variable is called t and represents time. However, in general, it doesn’t have to represent time. INDEPENDENT VARIABLE
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LOGO Thank you for your attention
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