As seen in Eq. (8), enthalpy is a s

As seen in Eq. (8), enthalpy is a state function of two variables while the first term (∂h/∂P∙dP) on the right side of Eq. (8) was only considered in Eq. (2). Enthalpy change according to temperature change (∂h/∂T∙dT) was ignored and the controller underestimated the cooling capacity increment.
เห็นใน Eq. (8), ความร้อนแฝงมีฟังก์ชันสถานะของสองตัวแปรขณะระยะแรก (∂h ∂P∙dP) บนฝั่งขวาของ Eq. (8) เท่านั้นที่ถือใน Eq. (2) ความร้อนแฝงเปลี่ยนแปลงตามการเปลี่ยนแปลงอุณหภูมิ (∂h ∂T∙dT) ได้ถูกละเว้น และตัวควบคุม underestimated เพิ่มกำลังระบายความร้อน

ผลลัพธ์ (อังกฤษ) 1:

As seen in Eq. (8), enthalpy is a state function of two variables while the first term (∂h/∂P∙dP) on the right side of Eq. (8) was only considered in Eq. (2). Enthalpy change according to temperature change (∂h/∂T∙dT) was ignored and the controller underestimated the cooling capacity increment.See in the Eq: (8), enthalpy is a function of two variables, while the first phase (dP P∙ ∂ ∂ h) on the right side of Eq: (8) only in Eq. (2) enthalpy change according to the change in temperature (dT T∙ ∂ ∂ h) has been ignored and underestimated controller cooling capacity.

ผลลัพธ์ (อังกฤษ) 2:

As seen in Eq. (8), enthalpy is a state function of two variables while the first term (∂h / ∂P ∙ dP) on the right side of Eq. (8) was only considered in Eq. (2). Enthalpy change according to temperature change (∂h / ∂T ∙ dT) was ignored and the controller underestimated the cooling capacity increment.
seen in Eq. (8), latent heat is a function of two variables in the first stage (∂h ∂. P ∙ dP) on the right side of Eq. (8) only holds in Eq. (2) heat varies according to temperature changes (∂h ∂T ∙ dT) was ignored and control underestimated. Increased cooling

ผลลัพธ์ (อังกฤษ) 3:

As seen in Eq. (8), enthalpy is a state function of two variables while the first term (∂ H / ∂ P ∙ dP) on the right side of. Eq. (8) was only considered in Eq. (2). Enthalpy change according to temperature change (∂ H / ∂ T ∙ dT) was ignored and the controller. Underestimated the cooling capacity increment.
seen in Eq. (8),Latent heat has the function of two variables, while the phase state (∂ h ∂ P ∙ dP) on the right side of the Eq. (8) only to hold in Eq.(2) latent heat change according to temperature changes (∂ h ∂ T ∙ dT) has been ignored and control underestimated increase cooling.