Use integration by parts to evaluate the following integral. \( \int_{-\infty}^{-6} \theta e^{\theta} d \theta \)
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To evaluate the integral \( \int_{-\infty}^{-6} \theta e^{\theta} d\theta \) using integration by parts, we first set: - \( u = \theta \) which gives \( du = d\theta \) - \( dv = e^{\theta} d\theta \) which gives \( v = e^{\theta} \) Now, applying the integration by parts formula \( \int u \, dv = uv - \int v \, du \): \[ \int \theta e^{\theta} d\theta = \theta e^{\theta} - \int e^{\theta} d\theta \] Calculating the integral: \[ \int e^{\theta} d\theta = e^{\theta} + C \] Thus, we have: \[ \int \theta e^{\theta} d\theta = \theta e^{\theta} - e^{\theta} + C = e^{\theta}(\theta - 1) + C \] Now, we evaluate the definite integral: \[ \int_{-\infty}^{-6} \theta e^{\theta} d\theta = \left[e^{\theta}(\theta - 1) \right]_{-\infty}^{-6} \] Evaluating at the limits: At \(\theta = -6\): \[ e^{-6}(-6 - 1) = e^{-6}(-7) = -7e^{-6} \] As \(\theta \to -\infty\): \[ \theta e^{\theta} \to 0 \text{ (since \( e^{\theta} \text{ goes to } 0 \text{ faster than } \theta \text{ goes to } -\infty \))} \] Thus: \[ \int_{-\infty}^{-6} \theta e^{\theta} d\theta = \left[0 - (-7e^{-6})\right] = 7e^{-6} \] So the final result is: \[ \int_{-\infty}^{-6} \theta e^{\theta} d\theta = 7e^{-6} \]