Interpretación de la relación presión-flujo en la hipertensión arterial pulmonar idiopática

Objetivo: Conocer más de la relación presión arterial pulmonar media/índice cardiaco y sus perfiles en enfermos con hipertensión arterial pulmonar idiopática. Métodos: La presión arterial pulmonar media/índice cardiaco y la presión extrapolada al eje de cero flujo se obtuvo en 40 enfermos respirando aire ambiente, oxígeno 99.5% e hidralazina. Se obtuvieron dos grupos de acuerdo a criterios de "respuesta vasodilatadora aguda", respondedores (n = 20) y no respondedores (n = 20). Se analizó este criterio versus el propuesto por la Task Force de la Sociedad Europea de Cardiología en la población respondedora. Resultados: La presión arterial pulmonar media/Índice cardiaco se ubicó de forma anormal en el diagrama de presión-flujo de la cohorte total, (p < 0.01). Sin alteraciones en el intercambio gaseoso o mecánica pulmonar. Para los enfermos respondedores versus no respondedores, la pendiente fue anormal 2.2 (95%IC:1.1-3.3) vs. 5.89 (95%IC:4.69-7.11) mm Hg/L min/m² e incremento de la presión extrapolada al eje de cero flujo (38.2 ± 7.5 a 66.3 ± 7.5 mm Hg, p < 0.01). Sin diferencias con oxígeno al 99.5%. Con vasodilatador, la presión arterial pulmonar media disminuyó (52.1 ± 9.5 a 40 ± 5.5 mm Hg, p < 0.01) vs. no se modificó (96.2 ± 8.5 vs. 90 ± 7.5 mmHg, p = 0.3), pendiente 1.15 (95%IC:0.68-1.62) vs. 1.28 (95%IC:0.78-1.78) mmHg/Lmin/m², la presión extrapolada al eje de cero flujo no cambió vs. incrementó (69.4 ± 7.8 a 85.1 ± 8.5 mm Hg, p < 0.01), en relación al control. En no respondedores con vasodilatador, la presión arterial pulmonar media/índice cardiaco (90 ± 7.5 mmHg, pendiente:1.28; 95%IC: 0.78 - 1.78 mm Hg/L min/m²) fue diferente al comparar respondedores con menor o mayor de 40 mm Hg de presión arterial pulmonar media. Presiones 34 ± 3 vs. 45 ± 4 mm Hg y pendientes 1.14 (95%IC: 0.67 -1.61 vs. 2.22 (95%IC: 1.35 - 3.09 mm Hg/L min/m²), respectivamente p < 0.01. Conclusiones: Las anormalidades de la relación presión arterial pulmonar media/Índice cardiaco reflejan el incremento de las resistencias vasculares pulmonares reales a nivel arteriolar pulmonar en enfermos con hipertensión arterial pulmonar idiopática. Ambos criterios de respuesta vasodilatadora aguda son de utilidad para identificar respondedores y no, en esta población de enfermos

Impacto de la maniobra de inspiración profunda en el intercambio gaseoso del sujeto con obesidad severa e hipertensión arterial pulmonar asociada a síndrome de Eisenmenger

La obesidad y el síndrome de Eisenmenger son entidades ampliamente estudiadas. Sin embargo, su asociación es inusual y no informada. Ambas cursan con alteraciones del intercambio gaseoso de grado variable. En la obesidad severa son atribuidas a trastornos en la relación ventilación/perfusión y al cortocircuito venoarterial pulmonar que dependen del volumen pulmonar. En el síndrome de Eisenmenger con obesidad severa, esta dependencia se desconoce. Material y métodos: Se estudiaron 28 sujetos obesos pareados por índice de masa corporal > 30 kg/m². Asignados a dos grupos, obesos con síndrome de Eisenmenger y obesos sin el síndrome. Se acotaron variables clínicas, función respiratoria, ecocardiografía y del intercambio gaseoso pre y posterior a la maniobra de inspiración profunda. Análisis estadístico: Las variables se expresaron con media ± desviación estándar. Se utilizó la prueba f de Student pareada y la correlación de Pearson, para las diferencias y la asociación de variables en los grupos. La significación estadística se estableció con p < 0.05. Resultados: La edad en cada grupo fue: 48.57 ± 10.32 vs 60.86 ± 10.47 años, p < 0.004 respectivamente. Presión arterial pulmonar sistólica 104.36 ± 37 vs 50.1 ± 12 mm Hg, p < 0.001. La presión arterial de oxígeno en reposo y maniobra de inspiración profunda en cada grupo: 51.64 ± 6.38 vs 57 AA ± 11, p<0.188 y 56.29 ± 11.15 vs 72 ± 11.83, p< 0.001; cortocircuito venoarterial 13.50 ± 3.66 vs 13.07 ± 4.84, p < 0.767 y 9.21 ± 3.77 vs 6.5 ± 2.28, p < 0.001; gradiente alvéolo-arterial de oxígeno 271.14 ± 79.92 vs 243.79 92.07, p < 0.001, respectivamente. Conclusión: En los sujetos obesos con síndrome de Eisenmenger no hubo mejoría significativa en el intercambio gaseoso con la maniobra de inspiración profunda

Left and right ventricular power: outputs are the strongest hemodynamic correlates to allow identification of acute responders to vasodilator treatment in idiopathic pulmonary arterial hypertension

Introduction: Despite the prognostic importance of traditionally derived measurements, the significance of right heart catheterization (RHC) remains controversial. Thus, a continued search for hemodynamic markers that define better responsive patients is required. Since, right ventricular failure is the most fatal pathway, right (RVPO) and left (LVPO) ventricular power output are parameters that could provide input for a better understanding of the hemodynamics involved in idiopathic pulmonary artery hypertension (IPAH). Method: We retrospectively analyzed how demographics and outcome correlate with hemodynamics to identify responders among IPAH patients. Results: Ninety patients fulfilled the following criteria for inclusion in this study: (1) complete RHC at baseline; (2) an acute evaluation for vasodilators (AEFV, including a positive response, that is, an increase in CO, a decrease in both mPAP and pulmonary vascular resistance &#8805; 20% from baseline, respectively); and (3) a long-term follow-up under accepted IPAH treatments. If RVPO decreased (p < 0.001) and LVPO increased (p < 0.012) during AEFV, it is considered that these findings reinforce our ability to identify responders; that is, patients that remained as responders after 6.4 ± 3 years under nifedipine treatment (37.7% of the studied IPAH population). After multivariate analysis, age, RVPO, and LVPO remained as independent variables (OR = 0.927, 95%CI: 0.87-0.98, p = 0.01; OR = 0.114, 95%CI: 0.00-0.91, p = 0.045; and OR = 171.5, 95% CI: 5.3-549, p = 0.004, respectively) when estimating the probability of being a responder. On this basis, an equation was derived to identify responders among IPAH patients, where the probability of being a responder = 1.0196-0.0631 (age) - 4.7693 (RVPO) + 3.8152 (LVPO), ROC: 0.76, 95% CI: 0.63-0.89; p = 0.001. Conclusion:based on the proposed equation, LVPO and RVPO could be used for the identification of responders among IPAH patients

Reflexiones médicas a propósito de un caso de tromboembolia pulmonar en el embarazo

La mortalidad materna en el mundo es aún alta. La tromboembolia pulmonar como causa de muerte ocupa el segundo lugar en países desarrollados. En Latinoamérica, la frecuencia informada es de 0.6%, lo cual contrasta con la señalada para países desarrollados (14.9%). Esta diferencia puede estar relacionada a sesgos de información. Por tal motivo se revisó la información actual del tema y presentamos un breve caso clínico de una mujer quien presentó evento de tromboembolia pulmonar en la semana 30 del embarazo; el manejo adecuado de la misma, permitió la supervivencia materna y fetal

ICU-Acquired Pneumonia Is Associated with Poor HealthPost-COVID-19 Syndrome

Background. Some patients previously presenting with COVID-19 have been reported to develop persistent COVID-19 symptoms. While this information has been adequately recognised and extensively published with respect to non-critically ill patients, less is known about the incidence and factors associated with the characteristics of persistent COVID-19. On the other hand, these patients very often have intensive care unit-acquired pneumonia (ICUAP). A second infectious hit after COVID increases the length of ICU stay and mechanical ventilation and could have an influence on poor health post-COVID 19 syndrome in ICU-discharged patients. Methods: This prospective, multicentre, and observational study was carrid out across 40 selected ICUs in Spain. Consecutive patients with COVID-19 requiring ICU admission were recruited and evaluated three months after hospital discharge. Results: A total of 1255 ICU patients were scheduled to be followed up at 3 months; however, the final cohort comprised 991 (78.9%) patients. A total of 315 patients developed ICUAP (97% of them had ventilated ICUAP). Patients requiring invasive mechanical ventilation had more persistent post-COVID-19 symptoms than those who did not require mechanical ventilation. Female sex, duration of ICU stay, development of ICUAP, and ARDS were independent factors for persistent poor health post-COVID-19. Conclusions: Persistent post-COVID-19 symptoms occurred in more than two-thirds of patients. Female sex, duration of ICU stay, development of ICUAP, and ARDS all comprised independent factors for persistent poor health post-COVID-19. Prevention of ICUAP could have beneficial effects in poor health post-COVID-1

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s= \sqrt{s} = 5.02 TeV

The inclusive jet cross section is measured as a function of jet transverse momentum $p_{\mathrm{T}}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} =$ 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4$\,\text{pb}^{-1}$. The jets are reconstructed with the anti-$k_{\mathrm{T}}$ algorithm using a distance parameter of $R=$ 0.4, within the rapidity interval $|y| <$ 2, and across the kinematic range 0.06 $< p_{\mathrm{T}} <$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$.The inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$