The bulk modulus (K) is defined as the ratio of the pressure change (Δp) applied to a material to the resulting relative volume change (ΔV/V) that it undergoes.
Mathematically, K is given by the equation:
K = -V(dP/dV)
where V is the initial volume of the material, P is the pressure, and dP/dV represents the derivative of P with respect to V.
To derive this equation, we start with a bar of initial volume V0 and apply a pressure P to it, resulting in a change in volume ΔV. The relationship between pressure and volume change is given by:
(dP/dV) = -K/V
where K/V represents the bulk modulus of the material.
Rearranging the equation, we have:
(dP/dV) * V = -K
Integrating both sides with respect to V, we get:
∫(dP/dV) * V dV = -∫K dV
Simplifying, we have:
∫P dV = -K * ∫dV
Integrating, we obtain:
PV = -KV + C
where C is the constant of integration.
Rearranging the equation, we have:
KV + PV = C
Since P is the external pressure and ΔV is the change in volume, we can write the equation as:
K(V0 + ΔV) + P(V0 + ΔV) = C
Expanding and rearranging the equation, we get:
KV0 + KΔV + PV0 + PΔV = C
Since C is a constant, KV0 + PV0 = C.
Substituting this value back into the equation, we have:
KΔV + PΔV = 0
Factoring out ΔV, we obtain:
(ΔV)(K + P) = 0
Since ΔV cannot be zero, we must have:
K + P = 0
Thus, we find that the bulk modulus (K) is given by:
K = -P
Therefore, the bulk modulus (volume modulus of elasticity) for a bar subjected to pressure P is equal to the negative of the applied pressure.
Derive the bulk modulus (volume modulus of elasticity) for a bar subjected under pressure p.
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